ID |
Date |
Author |
Subject |
419
|
Thu Nov 22 07:01:36 2018 |
AT | PID high mass seting (165Pm) - RIBF148 |
PID plot for the high mass setting (165Pm), run 2018, rare earth peak experiment.
Partial statistics (~30h) from identification at F7.
Please use for internal reports about the BRIKEN activities. |
Attachment 1: F7pid_RIBF148_165PmSetting_labels.png
|
|
418
|
Tue Nov 6 21:51:54 2018 |
NT Brewer | New D4Off.conf for HV also on github |
------ --------------- --------- ----- ---- ------- ------- ------ ------ ------------- |
0 192.168.13.239 0 0 PA1 1450 0.0001 50 10 1 |
0 192.168.13.239 1 0 PA2 1450 0.0001 50 10 1 |
0 192.168.13.239 2 0 PA3 1550 0.0001 50 10 1 |
0 192.168.13.239 3 0 PA4 1550 0.0001 50 10 1 |
0 192.168.13.239 4 0 PA5 1550 0.0001 50 10 1 |
0 192.168.13.239 5 0 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 6 0 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 7 0 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 0 1 PA6 1200 0.0001 50 10 1 |
0 192.168.13.239 1 1 PA7 1750 0.0001 50 10 1 |
0 192.168.13.239 2 1 PA8 1750 0.0001 50 10 1 |
0 192.168.13.239 3 1 PA9 1750 0.0001 50 10 1 |
0 192.168.13.239 4 1 PA10 1750 0.0001 50 10 1 |
0 192.168.13.239 5 1 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 6 1 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 7 1 OFF 0 0.0001 50 10 0 |
0 192.168.13.239 0 3 OFF 3000 0.0001 2 5 0 |
0 192.168.13.239 1 3 OFF 3000 0.0001 2 5 0 |
0 192.168.13.239 2 3 OFF 3000 0.0001 2 5 0 |
0 192.168.13.239 3 3 OFF 3000 0.0001 2 5 0 |
0 192.168.13.239 4 3 G70 2500 0.0001 2 5 1 |
0 192.168.13.239 4 3 G71 2500 0.0001 2 5 1 |
0 192.168.13.239 6 3 G72 2500 0.0001 2 5 1 |
0 192.168.13.239 7 3 G73 2500 0.0001 2 5 1 |
================================================= |
Everything below type = -1 is treated as a comment |
(Clover Names are DetectorName+(0,1,2,3=Black,Red/Orange,Green,Blue) |
type = 0 => MPOD HV modules => accessed thru snmp |
type = 1 => CAEN x527 HV modules => accessed thru CAENHVwrapper |
With MPOD one can use IP address and channel numbers based on slot occupation |
With CAEN one needs IP address and SLOT and CHAN |
Type IP address Slot Chan Name vSet iSet uRamp dRamp Switch On/Off |
------ -------------- ---- ---- -------------- ------ ------ ------ ------ ------------- |
0 192.168.13.239 0 3 D40 3000 0.5 2 5 0 |
0 192.168.13.239 1 3 D41 3000 0.5 2 5 0 |
0 192.168.13.239 2 3 D42 3000 0.5 2 5 0 |
0 192.168.13.239 3 3 D43 3000 0.5 2 5 0 |
0 192.168.13.239 4 3 G70 2500 0.5 2 5 0 |
0 192.168.13.239 5 3 G71 3000 0.5 2 5 0 |
0 192.168.13.239 6 3 G72 2500 0.5 2 5 0 |
0 192.168.13.239 7 3 G73 2500 0.5 2 5 0 |
-1
Type IP address channel slot name voltage Current RampUp RampDn Switch On/Off |
|
417
|
Mon Nov 5 22:47:40 2018 |
AT, JR, FM, PA | Low threshold, 252Cf, z=0cm, perpendicular 0 deg |
252Cf at z=0cm, i.e 0 cm from the center of the detector, source axis perpendicular at 0 deg
Low threshold.
18/11/06 START:08:00
18/11/06 STOP: 09:11
** Configuration file:
181030_Conf_BrikenFull_LowThrAdj_masterCLK.xlsx
ROOT file:
181106_0800_252Cf_z0cm_nopulser_0911.root
DLT files:
181106_0800_252Cf_z0cm_nopulser_155.dlt
181106_0800_252Cf_z0cm_nopulser_156.dlt
181106_0800_252Cf_z0cm_nopulser_157.dlt
Comment:
- Pulser OFF, using configuration file 181030_Conf_BrikenFull_LowThrAdj_masterCLK.xlsx
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed.
- In the online in RateBRIKEN a weird fluctuation is observed (screenshot, attachement 1) |
Attachment 1: Screenshot_from_2018-11-06_08-32-50.png
|
|
416
|
Mon Nov 5 21:24:20 2018 |
AT, JR, FM, PA | Low threshold, 252Cf, z=25cm, perpendicular 90 deg |
252Cf at z=25cm, i.e 25 cm from the center of the detector, source axis perpendicular at 90 deg
Low threshold.
18/11/06 START: 06:25
18/11/06 STOP: 07:45
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181106_0625_252Cf_z25cm_0745.root
DLT files:
181106_0625_252Cf_z25cm_153.dlt
181106_0625_252Cf_z25cm_154.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
415
|
Mon Nov 5 19:55:20 2018 |
AT, JR, FM, PA | Low threshold, 252Cf, z=0cm, perpendicular 90 deg |
252Cf at z=0cm, i.e 0 cm from the center of the detector, source axis perpendicular at 90 deg
Low threshold.
18/11/06 START:04:56
18/11/06 STOP: 06:16
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181106_0456_252Cf_z0cm_0616.root
DLT files:
181106_0456_252Cf_z0cm_150.dlt
181106_0456_252Cf_z0cm_151.dlt
181106_0456_252Cf_z0cm_152.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
414
|
Mon Nov 5 18:52:54 2018 |
MW, KR | suspicious clover G7 temp sensor |
Quote: |
We observed 6 pm LN2 filling of both clovers on Monday Nov 5th.
D4 went full within reasonable time of below 10 minutes.
Filling of G7 was stopped by "emergency sensor" after about 15 minutes of filling.
Likely the temp sensor at the LN2 overflow pipe of G7 should be changed.
The clock at LN2 fill system is off by about 25 minutes (filling comes later than set at the control unit.)
|
"The clock at LN2 fill system is off by about 25 minutes (filling comes later than set at the control unit.)"
Yes, This is how it always was.
"Filling of G7 was stopped by "emergency sensor" after about 15 minutes of filling. Likely the temp sensor at the LN2 overflow pipe of G7 should be changed."
You can put this on a different line of the fill system.... |
413
|
Mon Nov 5 18:05:48 2018 |
AT, JR, FM, PA | Low threshold, 252Cf, z=25cm, perpendicular 0 deg |
252Cf at z=25cm, i.e 25 cm from the center of the detector, source axis perpendicular
Low threshold.
18/11/06 START: 03:18
18/11/06 STOP: 04:39
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181106_0318_252Cf_z25cm_0439.root
DLT files:
181106_0318_252Cf_z25cm_148.dlt
181106_0318_252Cf_z25cm_149.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
412
|
Mon Nov 5 16:43:43 2018 |
FM, PA, | Low threshold, 252Cf, z=25cm, Parallel downstream |
252Cf at z=25cm, i.e 25 cm from the center of the detector, source axis parallel downstream
Low threshold.
18/11/06 START: 01:43
18/11/06 STOP: 03:03
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181106_0143_252Cf_z25cm_0303.root
DLT files:
181106_0143_252Cf_z25cm_146.dlt
181106_0143_252Cf_z25cm_147.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
411
|
Mon Nov 5 15:10:43 2018 |
FM, PA, | Low threshold, 252Cf, z=15cm, Parallel downstream |
252Cf at z=15cm, i.e 15 cm from the center of the detector, source axis parallel downstream
Low threshold.
18/11/06 START: 00:10
18/11/06 STOP: 01:32
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181106_0010_252Cf_z15cm_0132.root
DLT files:
181106_0010_252Cf_z15cm_143.dlt
181106_0010_252Cf_z15cm_144.dlt
181106_0010_252Cf_z15cm_145.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
410
|
Mon Nov 5 13:43:57 2018 |
FM, PA | Low threshold, 252Cf, z=0cm, Parallel downstream |
252Cf at z=0cm,ie center of moderator, source axis parallel downstream
Low threshold.
18/11/05 START: 22:46
18/11/05 STOP: 00:01
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181105_2245_252Cf_z0cm_0001.root
DLT files:
181105_2245_252Cf_z0cm_140.dlt
181105_2245_252Cf_z0cm_141.dlt
181105_2245_252Cf_z0cm_142.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
409
|
Mon Nov 5 12:04:08 2018 |
FM, PA, AT | Low threshold, 252Cf, z=15cm, Perpendicular 0deg |
252Cf at z=15cm,ie center of moderator, source axis perpendicular at 0deg (typical orientation)
Low threshold.
18/11/05 START: 21:05
18/11/05 STOP: 22.30
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181105_2105_252Cf_z15cm_2230.root
DLT files:
181105_2105_252Cf_z15cm_137.dlt
181105_2105_252Cf_z15cm_138.dlt
181105_2105_252Cf_z15cm_139.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
408
|
Mon Nov 5 09:59:36 2018 |
MW, KR | suspicious clover G7 temp sensor |
We observed 6 pm LN2 filling of both clovers on Monday Nov 5th.
D4 went full within reasonable time of below 10 minutes.
Filling of G7 was stopped by "emergency sensor" after about 15 minutes of filling.
Likely the temp sensor at the LN2 overflow pipe of G7 should be changed.
The clock at LN2 fill system is off by about 25 minutes (filling comes later than set at the control unit.)
|
407
|
Mon Nov 5 09:32:00 2018 |
FM, JR, PA, AT | Low threshold, 252Cf, z=0cm, Perpendicular 0deg |
252Cf at z=0cm,ie center of moderator, source axis perpendicular at 0deg (typical orientation)
Low threshold.
18/11/05 START: 18:50
18/11/05 STOP: 20:45
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181105_1850_252Cf_z0cm_2045.root
DLT files:
181105_1850_252Cf_z0cm_133.dlt
181105_1850_252Cf_z0cm_134.dlt
181105_1850_252Cf_z0cm_135.dlt
181105_1850_252Cf_z0cm_136.dlt
Comment:
- Clovers are placed inside the moderator, front face ~5mm from AIDA hole border.
- AIDA not inside the moderator.
- In beam PE shielding placed. |
406
|
Mon Nov 5 06:46:30 2018 |
KR, YR, MW, JLT, ... | Clover check |
With detectors still on the floor we check signals and found
that D4 gives no signal with PA power. Two power supplies/cables were checked.
The detector was still working just before Jungclaus experiment. In July it was working.
Temperature monitors OK: 76-80 units
We mount both CLovers in position and make all connections.
We apply HV and check the resolution of G7.
Source: 152Eu
File: 181105_1550_CloverCheck_152Eu.root
As can be seen in the attached figure the calibration used last year
is still pretty good
Resolution @ 1408 keV
G7 black: 2.75keV
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 Constant 6.57807e+02 1.35347e+01 4.63240e-02 -7.68897e-07
2 Mean 1.40766e+03 1.96681e-02 6.71225e-04 5.14533e-03
3 Sigma 1.16983e+00 1.52231e-02 1.41407e-05 -1.28285e-02
G7 red: 2.97keV
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 Constant 5.60626e+02 1.17448e+01 3.69357e-02 1.06287e-06
2 Mean 1.40659e+03 2.29862e-02 6.70713e-04 1.36869e-04
3 Sigma 1.26305e+00 1.62145e-02 1.30239e-05 -1.44151e-02
G7 green: 2.75keV
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 Constant 7.87830e+02 1.48889e+01 3.68407e-02 5.57077e-06
2 Mean 1.40597e+03 1.75988e-02 6.70417e-04 -2.47334e-03
3 Sigma 1.17167e+00 1.41220e-02 9.59214e-06 1.55873e-02
G7 blue: 2.73keV
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 Constant 4.99089e+02 1.19364e+01 -6.77351e-03 -4.15987e-06
2 Mean 1.40489e+03 2.17210e-02 2.57134e-05 2.38923e-03
3 Sigma 1.16057e+00 1.73778e-02 3.14777e-06 2.01018e-02
FWHM: |
Attachment 1: Screenshot_from_2018-11-05_15-57-40.png
|
|
Attachment 2: Screenshot_from_2018-11-05_16-23-12.png
|
|
405
|
Fri Nov 2 14:18:54 2018 |
JLT | 136Sn at ZDS |
Measurement of neutron background while
Jungclaus experiment is running
Secondary beam 136Sn at ~140MeV/u, Be target, 136Sn in the ZDS
Start: 23:17
Stop:
DLT: 181102_2317_136Sn_Be_136Sn_131.dlt
Online: 181102_2338_136Sn_Be_136Sn.root
F11 Rate: 7 kcps
BRIKEN Rate: 3.2 kcps |
404
|
Fri Nov 2 01:07:21 2018 |
JLT | 134Sn/133In on ZDS |
Measurement of neutron background while
Jungclaus experiment is running
Secondary beam:
134Sn at ~140MeV/u, Au target, 134Sn in the ZDS
after 2:00 AM: 134Sn at ~140MeV/u, Be target, 133In in the ZDS
Long run
Start: 17:37
Stop: 10:08 (2018/11/02)
tmeas=59400s (16.5h)
DLT: NO
Online: 181102_1008_134Sn_AuBe_134Sn133In.root
F11 Rate: 11.5 kcps
BRIKEN Rate: 3 kcps |
Attachment 1: Screenshot_from_2018-11-02_10-17-34.png
|
|
Attachment 2: Screenshot_from_2018-11-02_10-20-20.png
|
|
Attachment 3: Screenshot_from_2018-11-02_10-21-50.png
|
|
403
|
Wed Oct 31 03:41:33 2018 |
JLT | 134Sn at ZDS |
Measurement of neutron background while
Jungclaus experiment is running
Secondary beam 134Sn at ~140MeV/u, Au target, 134Sn in the ZDS
Start: 12:40
Stop: 13:01
DLT: 181031_1240_134Sn_Au_134Sn_129.dlt
Online: 181031_1301_134Sn_Au_134Sn.root
F11 Rate: 11.5 kcps
BRIKEN Rate: 3 kcps |
402
|
Wed Oct 31 00:36:34 2018 |
JLT | 133In at ZDS |
Measurement of neutron background while
Jungclaus experiment is running
Secondary beam 134Sn at XXMeV, Be target, 133In i the ZDS
Start: 9:35
Stop: 9:55
DLT: 181031_0935_134Sn_Be_133In_127.dlt
Online:181031_0955_134Sn_Be_133In.root
F11 Rate: 11.5 kcps
BRIKEN Rate: 3 kcps |
401
|
Tue Oct 30 01:01:42 2018 |
JLT, AA | Adjustment of 3He thresholds |
Background with BigRIPS+ZD already working
No pulser
After adjustment of thresholds the rate of BRIKEN noise
was reduced to 4.5kHz
The corresponding configuration file is:
181030_Conf_BrikenFull_LowThrAdj_masterCLK.xlsx
To be decided if we want to reduce further the noise rate
We also changed the calibration of the F11 plastic to have it in the histogram range
F11_PL_R_LG: 2.73 -> 1.0
F11_PL_L_LG: 2.32 -> 2.0
Further adjustment of few channels: Now noise rate is 2.7kHz
(2018/10/30 15:45) |
Attachment 1: 181030_Conf_BrikenFull_LowThrAdj_masterCLK.xlsx
|
Attachment 2: Screenshot_from_2018-10-30_16-22-32.png
|
|
400
|
Mon Oct 29 12:08:12 2018 |
JR, JA, AT | Background |
Background was measurement
Pulser: NO
DLT: No
Online:
Start:21:07
Stop:
Comment: V2A8C9 contains now the 10Hz clock signal coming from
the same section of the clock where the 100Hz sync signal is extracted.
It will be there even if we inhibit the pulser signals to the preamps
SYNC pulser is 200Hz because
the gate generator produces double peaks from the 100Hz clock
v1a6c13-16 had a configuration error (Trigger window to short)
It's corrected at 14:55 (2018/10/30) on file 181030_Conf_BrikenFull_LowThrAdj_masterCLK.xlsx . |
399
|
Sun Oct 28 07:41:03 2018 |
AT, JA, AA | Background |
Dacq was reinitialized
Background was measurement
Pulser: YES
DLT: No
Online: 181029_1640prevday_1723_Bkg_Pulser.root
Start:16:40
Stop: 17:23
Comment: We started a Ge filling manually, to check if the funny behavior of the
Corr_BR_BR can be reproduced. It remained clean. So we do not yet what caused the
funny behavior.
Funny behavior definition: periodic peaks appeared in the Corr_BR_BR file
The synch software problem will be solved tomorrow.
Tomorrow definition: a mystical land were 99% of all human productivity, motivation
and achievement is stored |
398
|
Fri Oct 26 15:15:55 2018 |
JA, ATS, ATD, JLT, AA | Background measurements |
No pulser (inhibit in clock)
DLT: 181026_2244_Bkg_NoPulser_114.dlt
Online: 181026_2259_Bkg_NoPulser.root
TTree: 181026_2244_Bkg_NoPulser_114.root
With pulser:
DLT: 181026_2305_Bkg_Pulser_115.dlt (erased)
Online: 181026_2314_Bkg_Pulser.root
TTree: no
VME crate reset
No pulser:
DLT: 181026_2324_Bkg_NoPulser_116.dlt
Online: 181026_2331_Bkg_NoPulser.root
We adjust all the thresholds reducing them
drastically to see the noise.
Overnight measurement:
Online: 181027_1137_BkgOverNight_NoPulser.root
Start measurements with DLT
No pulser:
Start: 11:42
Stop: 12:46
DLT: 181027_1142_Bkg_NoPulser_VeryLowThr_117.dlt
Online: 181027_1246_Bkg_NoPulser_VeryLowThr.root
Bckg rate:
Fit to RateBRIKEN= 0.340 cps
With pulser:
Start: 12:53
Stop: 14:08
DLT: 181027_1253_Bkg_Pulser_VeryLowThr_118.dlt & *_119.dlt
Online: 181027_1408_Bkg_Pulser_VeryLowThr.root
Bckg rate:
t(10Hz pulse)= 4458s, BRIKEN:2547 counts, Rate=0.571 cps
tube bkg (Integral(l830,1550))=885, net=1662counts, Rate=0.373cps
Fit to RateBRIKEN= 0.566 cps
252Cf source in the center
With pulser:
Start: 14:37
Stop: 16:51
DLT: 181027_1437_252Cf_Pulser_VeryLowThr_120.dlt Runs: 120-123
Online: 181027_1437_252Cf_z0cm_Pulser_VeryLowThr_1652.root
252Cf rate:
t(10Hz pulse)=7973.80 s, BRIKEN: 7.66289e+07 counts, Rate= 9610.09 cps
Fit to RateBRIKEN= 9594.69 cps
No pulser:
Start: 16:57
Stop: 18:47
DLT: 181027_1657_252Cf_NoPulser_VeryLowThr_124.dlt
Online:181027_1657_252Cf_z0cm_NoPulser_VeryLowThr_1847.root
Fit to RateBRIKEN=9591.79 cps
Background:
No Pulser:
DLT: No
Online: 181028_1056_BkgOverNight_NoPulser.root
With pulser:181028_1056_1641_Bkg_Pulser.root
DLT: No
Commments: Corr_BR_BR looks funny. It shows periodic peaks. Probably related to the
filling of the Ge detector. We will stop to check if it appears again |
397
|
Fri Oct 26 03:57:37 2018 |
ATS & JLT | Background |
Background BRIKEN control measurement
No DLT
2018/10/26
Start: 11:57
Stop: 14:00
ROOT file: 181026_1400_Bkg.root
Measurement re-started at 15:58 |
396
|
Fri Oct 26 03:31:33 2018 |
AT2 & JA | Test pulser effect on baseline |
We have tested possible change of the baseline in the digitizer due to the pulser connection. NO EFFECT has been
found!
Test for detector He086 ORNL:
He086_NoPulser_samples.png -> Without pulser, baseline around 1000
He086_Pulser_samples.png -> With pulser, baseline around 1000
Test for detector He001 UPC:
He001_Pulser_samples.png -> With pulser, baseline around 1200
He001_NoPulser_samples.png -> Without pulser, baseline around 1200
Test for detector He013 RIKEN:
He013_Pulser_samples.png -> With pulser, baseline around 850
He013_NoPulser_samples.png -> Without pulser, baseline around 850 |
Attachment 1: He086_NoPulser_samples.png
|
|
Attachment 2: He086_Pulser_samples.png
|
|
Attachment 3: He001_Pulser_samples.png
|
|
Attachment 4: He001_NoPulser_samples.png
|
|
Attachment 5: He013_Pulser_samples.png
|
|
Attachment 6: He013_NoPulser_samples.png
|
|
395
|
Fri Oct 26 03:24:25 2018 |
ATS & JLT | Background |
Background BRIKEN control measurement
No DLT
2018/10/26
Start: 10:00 aprox
Stop: 11:20
ROOT file: 181026_1120_Bkg.root |
394
|
Thu Oct 25 16:08:53 2018 |
ATS & JLT | Lead bricks |
Lead bricks in BRIKEN hole to protect AIDA |
393
|
Thu Oct 25 16:04:17 2018 |
ATS & JLT | Background |
Background BRIKEN control measurement
No DLT
2018/10/26
Start: 00:03
Stop: 09:46
ROOT file: 181026_0946_Bkg.root |
392
|
Thu Oct 25 09:32:25 2018 |
AT & AT | Low threshold, 252Cf, z=25cm, Perpendicular 90deg |
252Cf at z=25cm,ie 25 cm upstream the beam, source axis perpendicular at 90deg with respect to typical
orientation.
Low threshold.
18/10/25 START: 17:32
18/10/25 STOP: 23:30
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181025_1732_252Cf_z25cm_2330.root
DLT files:
181025_1732_252Cf_z25cm_109.dlt
181025_1732_252Cf_z25cm_110.dlt
181025_1732_252Cf_z25cm_111.dlt
181025_1732_252Cf_z25cm_112.dlt
181025_1732_252Cf_z25cm_113.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
****3He tubes 12 and 7 (RIKEN) were shifted 3cm aprox from their position upstream (CHECK DATA). |
391
|
Thu Oct 25 09:18:24 2018 |
ATS & JLT | F11 plastic |
F11 plastic (long plastic after MUSIC chamber)
connected to DACQ.
The connections were re-cabled and verified.
F11 plastic has 0.2mm thickness (check!)
Current HV: 2000V |
390
|
Thu Oct 25 09:07:00 2018 |
ATS & JLT | BRIKEN Calibration check |
We put the 252Cf source and check the aligment of 3He tubes gains:
File: 181025_1600_252Cf_gaincheck.root
All OK except 133, 35 and 140
He133: peak at 744keV
He135: peak at 783keV
He140: peak at 739keV
No gain correction applied at the moment but should be verified
before experiment |
389
|
Thu Oct 25 04:14:00 2018 |
AT & AT | Low threshold, 252Cf, z=25cm, Perpendicular 90deg |
252Cf at z=25cm,ie 25 cm upstream the beam, source axis perpendicular at 90deg with respect to typical
orientation.
Low threshold.
18/10/25 START: 12:13
18/10/25 STOP: 15:42
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181025_0213_252Cf_z25cm_1542.root
DLT files:
181025_0213_252Cf_z25cm_106.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
****** CHECK DATA, possible issue with the clock due to AIDA test. |
Attachment 1: 181025_0213_252Cf_z25cm.png
|
|
388
|
Thu Oct 25 00:53:43 2018 |
AT & AT | Low threshold, 252Cf, z=-25cm, Perpendicular 90deg |
252Cf at z=-25cm,ie 25 cm downstream the beam, source axis perpendicular at 90deg with respect to typical
orientation.
Low threshold.
18/10/25 START: 08:55
18/10/25 STOP: 12:05
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181025_0854_252Cf_zm25cm_1205.root
DLT files:
181025_0854_252Cf_zm25cm_103.dlt
181025_0854_252Cf_zm25cm_104.dlt
181025_0854_252Cf_zm25cm_105.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
387
|
Wed Oct 24 16:11:32 2018 |
AT & AT | Low threshold, 252Cf, z=-25cm |
252Cf at z=-25cm,ie 25 cm downstream the beam, source axis parallel.
Low threshold.
18/10/24 START: 00:12
18/10/25 STOP: 08:42
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181025_0012_252Cf_zm25cm_0842.root
DLT files:
181025_0012_252Cf_zm25cm_096.dlt
181025_0012_252Cf_zm25cm_097.dlt
181025_0012_252Cf_zm25cm_098.dlt
181025_0012_252Cf_zm25cm_099.dlt
181025_0012_252Cf_zm25cm_100.dlt
181025_0012_252Cf_zm25cm_101.dlt
181025_0012_252Cf_zm25cm_102.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
386
|
Wed Oct 24 11:28:42 2018 |
AT & AT | Low threshold, 252Cf, z=-25cm |
252Cf at z=-25cm,ie 25 cm downstream, source axis perpendicular, typical orientation.
Low threshold.
18/10/24 START: 19:31
18/10/25 STOP: 00:01
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181024_1930_252Cf_zm25cm_0001.root
DLT files:
181024_1930_252Cf_zm25cm_092.dlt
181024_1930_252Cf_zm25cm_093.dlt
181024_1930_252Cf_zm25cm_094.dlt
181024_1930_252Cf_zm25cm_095.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
385
|
Wed Oct 24 11:27:51 2018 |
AT & AT | Low threshold, 252Cf, z=10cm, source axis parallel |
252Cf at z=10cm, source axis parallel upstream to the beam.
Low threshold.
18/10/24 START: 15:44
18/10/24 STOP: 19:00
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181024_1544_252Cf_z10cm_1900.root
DLT files:
181024_1544_252Cf_z10cm_089.dlt
181024_1544_252Cf_z10cm_090.dlt
181024_1544_252Cf_z10cm_091.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
******* AT: By mistake duplicated entry from 385. |
384
|
Wed Oct 24 07:42:42 2018 |
AT & AT | Low threshold, 252Cf, z=10cm, source axis parallel |
252Cf at z=10cm, source axis parallel upstream to the beam.
Low threshold.
18/10/24 START: 15:44
18/10/24 STOP: 19:00
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181024_1544_252Cf_z10cm_1900.root
DLT files:
181024_1544_252Cf_z10cm_089.dlt
181024_1544_252Cf_z10cm_090.dlt
181024_1544_252Cf_z10cm_091.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
383
|
Wed Oct 24 03:49:01 2018 |
AT & AT | Low threshold, 252Cf, z=0cm |
252Cf at z=10cm, source axis perpendicular to beam axis, typical orientation.
Low threshold.
18/10/24 START: 11:50
18/10/24 STOP: 15:37
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181024_1150_252Cf_z10cm_1537.root
DLT files:
181024_1150_252Cf_z10cm_085.dlt
181024_1150_252Cf_z10cm_086.dlt
181024_1150_252Cf_z10cm_087.dlt
181024_1150_252Cf_z10cm_088.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
382
|
Mon Oct 22 16:54:10 2018 |
AT & AT | background, low threshold, No Pulser |
18/10/23 START: 00:53
18/10/24 STOP: 10:12
Background measurements. Checking noise!
Pulser is totally disconnected.
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
181023_0053_Nopulser_bckgn_1012.root
DLT files:
181023_0053_Nopulser_bckgn_084.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
***** NO neutron signals are observed without pulser (?!). Online plot provided. |
Attachment 1: 181023_0053_Nopulser_bckgn_1012.png
|
|
381
|
Mon Oct 22 11:42:50 2018 |
AT & AT | 252Cf, z=25cm, no clovers |
252Cf source placed using cardboard piece at z=25cm, source axis parallel upstream to the beam axis.
18/10/22 START: 19:44
18/10/22 STOP: 00:04
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181022_1944_252Cf_z25cm_SourceParAxis_0004.root
DLT:
181022_1944_252Cf_z25cm_SourceParAxis_081.dlt
181022_1944_252Cf_z25cm_SourceParAxis_082.dlt
181022_1944_252Cf_z25cm_SourceParAxis_083.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
380
|
Mon Oct 22 08:15:52 2018 |
AT & AT | 252Cf, z=15cm, no clovers |
252Cf source placed using cardboard piece at z=15cm, source axis parallel to the beam axis.
18/10/22 START: 16:15
18/10/22 STOP: 19:37
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181022_1615_252Cf_z15cm_SourceParAxis_1937.root
DLT:
181022_1615_252Cf_z15cm_SourceParAxis_078.dlt
181022_1615_252Cf_z15cm_SourceParAxis_079.dlt
181022_1615_252Cf_z15cm_SourceParAxis_080.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
379
|
Mon Oct 22 03:11:32 2018 |
AT & AT | background, high threshold, Pulser UPC |
18/10/22 START: 11:13
18/10/22 STOP: 15:59
Background measurements. Checking noise!
Pulser is connected to UPC tubes. RIKEN and ORNL tubes WITHOUT pulser.
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
181020_1113_bckgn_pulserUPC_highThr_1559.root
DLT files:
181020_1113_bckgn_pulserUPC_highThr_077.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
378
|
Sun Oct 21 15:16:40 2018 |
AT & AT | background, high threshold, Pulser RIKEN+ORNL |
18/10/21 START: 23:16
18/10/22 STOP: 11:06
Background measurements. Checking noise!
Pulser is connected to RIKEN and ORNL tubes. UPC tubes WITHOUT pulser.
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
181020_2030_bckgn_pulserRikenOrnl_highThr_1106.root
DLT files:
181020_2030_bckgn_pulserRikenOrnl_highThr_075.dlt
181020_2030_bckgn_pulserRikenOrnl_highThr_076.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
377
|
Sun Oct 21 11:18:31 2018 |
AT & AT | Low threshold, NO pulser, 252Cf, z=0cm |
18/10/21 START: 19:21
18/10/21 STOP: 23:04
252Cf at z=0cm, source axis perpendicular to beam axis, typical orientation.
Pulser is totally disconnected.
Low threshold.
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181019_2339_252Cf_z0cm_NOpulser_2304.root
DLT files:
181019_2339_252Cf_z0cm_NOpulser_072.dlt
181019_2339_252Cf_z0cm_NOpulser_073.dlt
181019_2339_252Cf_z0cm_NOpulser_074.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
**** There is a mistake in the time stamp of the name of the files, it says 181019_2339, it should be
181021_1921. This issue is corrected in the offline files. |
376
|
Sun Oct 21 08:58:23 2018 |
AT & AT | background, high threshold, NO pulser |
18/10/21 START: 16:58
18/10/21 STOP: 19:09
Background measurements. Checking noise!
Pulser is totally disconnected.
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
By mistake no online saved!
DLT files:
181021_1410_bckgn_NOpulser_highThr_071.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
375
|
Sun Oct 21 06:04:43 2018 |
AT & AT | background, high threshold |
18/10/21 START: 14:10
18/10/21 STOP: 16:41
Background measurements. Checking noise!
Pulser is connected to all preamps.
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
181021_1410_bckgn_pulser_highThr.root
DLT files:
181021_1410_bckgn_pulser_highThr_070.dlt
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
Attachment 1: 181021_1410_bckgn_pulser_highThr.png
|
|
374
|
Sun Oct 21 03:19:54 2018 |
AT & AT | background, high threshold |
18/10/20 START: 20:30 approx
18/10/21 STOP: 11:20
** Configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
181020_2030_bckgn_pulser_highThr.root
Comment:
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
373
|
Fri Oct 19 15:38:11 2018 |
AT & AT | 252Cf, z=0cm, no clovers, noise check individual tubes |
18/10/19 START: 23:39
18/10/20 STOP: 18:30
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181019_2339_252Cf_z0cm_1830.root
DLT:
181019_2339_252Cf_z0cm_050.dlt
181019_2339_252Cf_z0cm_051.dlt
181019_2339_252Cf_z0cm_052.dlt
181019_2339_252Cf_z0cm_053.dlt
181019_2339_252Cf_z0cm_054.dlt
181019_2339_252Cf_z0cm_055.dlt
181019_2339_252Cf_z0cm_056.dlt
181019_2339_252Cf_z0cm_057.dlt
181019_2339_252Cf_z0cm_058.dlt
181019_2339_252Cf_z0cm_059.dlt
181019_2339_252Cf_z0cm_060.dlt
181019_2339_252Cf_z0cm_061.dlt
181019_2339_252Cf_z0cm_062.dlt
181019_2339_252Cf_z0cm_063.dlt
181019_2339_252Cf_z0cm_064.dlt
181019_2339_252Cf_z0cm_065.dlt
181019_2339_252Cf_z0cm_066.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis parallel to the beam axis.
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
Noise check:
- He032, He034, He036, He038 have noise peak @ 15 keV (black = He032, red = He034, green = He036, blue = He038).
Tubes He031, 33,35 and 37 have not this peak. |
Attachment 1: Screenshot_from_2018-10-20_18-45-17.png
|
|
372
|
Fri Oct 19 11:45:12 2018 |
AT & AT | 252Cf, z=0cm, no clovers |
18/10/19 START: 19:46
18/10/19 STOP: 23:33
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
181019_1946_252Cf_z0cm_2333.root
DLT:
181019_1946_252Cf_z0cm_045.dlt
181019_1946_252Cf_z0cm_046.dlt
181019_1946_252Cf_z0cm_047.dlt
181019_1946_252Cf_z0cm_048.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis perpendicular to the beam axis,
rotated 90deg with respect to previous measurements.
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
371
|
Fri Oct 19 11:28:31 2018 |
AT & AT | 252Cf, z=0cm, no clovers, test online dead time |
During previous measurement a high dead time in the online was observed (50%). after restarting the crates and
the GASIFIC70, we resume the measurement. The conf file is
181016_Conf_BrikenFull.xlsx
18/10/19 START: 18:30
18/10/19 STOP: 19:32
ROOT file:181019_1926_252Cf_test.root
DLT:
181019_1926_252Cf_test_043.dlt
-------------------------------------
DACQ IS RESTARTED
The conf file is
181016_Conf_BrikenFull_2153_test_thr.xlsx
18/10/19 START: 19:34
18/10/19 STOP:
ROOT file: 181019_1934_252Cf_test.root
DLT:
181019_1934_252Cf_test_044.dlt
*** No significant differences between the two measurements.
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis perpendicular to the beam axis,
rotated 90deg with respect to previous measurements.
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding. |
370
|
Fri Oct 19 10:27:22 2018 |
AT & AT | 252Cf, z=0cm, no clovers (***** CHECK DATA) |
18/10/19 START: 18:25
18/10/19 STOP: 19:19
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file:
DLT:
181019_1825_252Cf_z0cm_042.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis perpendicular to the beam axis,
rotated 90deg with respect to previous measurements.
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
** A high dead time has been observed in the online (50%). The system is completely restarted for checking.
***** CHECK DATA, CHANGE OF CONFIGURATION WITHOUT RESTARTING GASIFIC70 |
369
|
Fri Oct 19 04:02:36 2018 |
AT & AT | 252Cf, z=0cm, no clovers (***** CHECK DATA) |
18/10/19 START: 12:05
18/10/19 STOP: 16:44
** Configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181019_1208_1643_252Cf_z0cm_038_041.root
DLT:
181019_1208_252Cf_z0cm_038.dlt
181019_1208_252Cf_z0cm_039.dlt
181019_1208_252Cf_z0cm_040.dlt
181019_1208_252Cf_z0cm_041.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis parallel to the beam axis.
- Clovers were placed outside the moderator
- AIDA not inside the moderator.
- Without In beam PE shielding.
-181019_1207_252Cf_z0cm_037.dlt was dummy
***** CHECK DATA, CHANGE OF CONFIGURATION WITHOUT RESTARTING GASIFIC70 |
368
|
Fri Oct 19 00:28:48 2018 |
AT2, JLT, SN | background measurement, no clovers |
18/10/19 START: 08:31
18/10/19 STOP: 10:50
Configuration file: 181016_Conf_BrikenFull.xlsx
ROOT file: 181019_1050_Bkg.root
DLT: 181019_0830_bckg_035.dlt
Comment:
- Clovers OUT of the moderator.
- AIDA not inside the moderator.
- Without In beam PE shielding.
Little noise in some tubes:
He039, He053, He121
We tried to improve the noise by moving cables around
but it didnt work. So we leave as it is.
***** CHECK DATA, CHANGE OF CONFIGURATION WITHOUT RESTARTING GASIFIC70 |
Attachment 1: Screenshot_from_2018-10-19_10-47-54.png
|
|
Attachment 2: Screenshot_from_2018-10-19_10-55-30.png
|
|
367
|
Thu Oct 18 15:24:40 2018 |
AT2, JLT, SN | 252Cf long measure, z=25cm beam upstream, no clovers |
18/10/18 START: 23:23
18/10/19 STOP: 08:23
** Use of other configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181018_2323_252Cf_z25cm_0823.root
DLT:
181018_2323_252Cf_z25cm_028.dlt
181018_2323_252Cf_z25cm_029.dlt
181018_2323_252Cf_z25cm_030.dlt
181018_2323_252Cf_z25cm_031.dlt
181018_2323_252Cf_z25cm_032.dlt
181018_2323_252Cf_z25cm_033.dlt
181018_2323_252Cf_z25cm_034.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=25cm beam upstream, source axis perpendicular to
the beam axis.
- Clovers OUT of the moderator.
- AIDA not inside the moderator.
- Without In beam PE shielding. |
366
|
Thu Oct 18 12:16:39 2018 |
AT2, JLT, SN | 252Cf long measure, z=15cm beam upstream, no clovers |
18/10/18 START: 20:20
18/10/18 STOP: 23:17
** Use of other configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181018_2020_252Cf_z15cm_2317.root
DLT:
181018_2020_252Cf_z15cm_025.dlt
181018_2020_252Cf_z15cm_026.dlt
181018_2020_252Cf_z15cm_027.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=15cm beam upstream, source axis perpendicular to
the beam axis.
- Clovers OUT of the moderator.
- AIDA not inside the moderator.
- Without In beam PE shielding. |
365
|
Thu Oct 18 08:21:18 2018 |
AT2, JLT, SN | 252Cf long measure, z=0cm, no clovers |
18/10/18 START: 17:22
18/10/18 STOP: 20:09
** Use of other configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181018_1722_252Cf_z0cm_2010.root
DLT:
181018_1722_252Cf_z0cm_021.dlt
181018_1722_252Cf_z0cm_022.dlt
181018_1722_252Cf_z0cm_023.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, source axis perpendicular to
the beam axis.
- Clovers WITHOUT the moderator.
- AIDA not inside the moderator.
- Without In beam PE shielding. |
364
|
Thu Oct 18 03:11:56 2018 |
AT & AT | bck meas |
18/10/18 START: 10:54
18/10/1X STOP: 14:02
** Use of other configuration file:
181016_Conf_BrikenFull.xlsx
ROOT file:
DLT: 181018_1054_Bck_018.dlt
Comment:
- Clovers inside the moderator, surface position 11.6/2 cm from the each one.
- AIDA not inside the moderator.
- Without in beam PE shielding.
- Working on Total Kinetic Energy Detector @ F11 (after F11 Music). |
363
|
Thu Oct 18 00:31:55 2018 |
AT & AT | 252Cf long measure, z=0cm, threshold 5% lower |
18/10/18 START: 08:31
18/10/18 STOP: 10:50
** Use of other configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181018_1050_252Cf_z0cm_lowThr.root
DLT:
191017_0831_252Cf_z0cm_lowThr_014.dlt
191017_0831_252Cf_z0cm_lowThr_015.dlt
191017_0831_252Cf_z0cm_lowThr_016.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, orientation of the source with its axis parallel to the beam axis, i.e. axis of the source upstream to the beam.
- 3He counters with a threshold 5% lower compared to previous measurement.
- Clovers inside the moderator, surface position 11.6/2 cm from the each one.
- AIDA not inside the moderator.
- Without in beam PE shielding. |
362
|
Wed Oct 17 14:11:18 2018 |
AT & AT | 252Cf long measure, z=0cm, threshold 5% lower |
18/10/17 START: 22:04
18/10/17 STOP: 08:18
** Use of other configuration file:
181016_Conf_BrikenFull_2153_test_thr.xlsx
ROOT file: 181017_2204_252Cf_z0cm_lowThr_0818.root
DLT:
181017_2204_252Cf_z0cm_lowThr_004.dlt
181017_2204_252Cf_z0cm_lowThr_005.dlt
181017_2204_252Cf_z0cm_lowThr_006.dlt
181017_2204_252Cf_z0cm_lowThr_007.dlt
181017_2204_252Cf_z0cm_lowThr_008.dlt
181017_2204_252Cf_z0cm_lowThr_009.dlt
181017_2204_252Cf_z0cm_lowThr_010.dlt
181017_2204_252Cf_z0cm_lowThr_011.dlt
181017_2204_252Cf_z0cm_lowThr_012.dlt
181017_2204_252Cf_z0cm_lowThr_013.dlt
Comment:
- 3He counters with a threshold 5% lower compared to previous measurement.
- 252Cf source placed at the center using cardboard piece, z=0cm, orientation of the source similar to past year
measurements, i.e. axis of the source perpendicular to the beam axis.
- Clovers inside the moderator, surface position 11.6/2 cm from the each one.
- AIDA not inside the moderator.
- Without in beam PE shielding. |
361
|
Wed Oct 17 09:20:20 2018 |
AT & AT | 252Cf long measure |
18/10/17 START: 18:16
18/10/17 STOP: 22:00
ROOT file: 181017_1816_252Cf_z0cm_2200.root
DLT:
181017_1816_252Cf_z0cm_000.dlt
181017_1816_252Cf_z0cm_001.dlt
181017_1816_252Cf_z0cm_002.dlt
181017_1816_252Cf_z0cm_003.dlt
Comment:
- 252Cf source placed at the center using cardboard piece, z=0cm, orientation of the source similar to past year
measurements, i.e. axis of the source perpendicular to the beam axis.
- Clovers inside the moderator, surface position 11.6/2 cm from the each one.
- AIDA not inside the moderator.
- Without in beam PE shielding. |
360
|
Tue Oct 16 09:00:02 2018 |
ATD & JLT | Background measurement overnight |
18/10/16 START: 16:56
18/10/17 STOP: 9:51
ROOT file: 181017_0951_BkgOverNight.root
Comment:
Tube 121 is noisier than the others (see fig).
Issue:
all the channels connected to PA3 and PA4
have twice the number of counts than the remaining channels (!?).
Actually the pulser counts.
Solution:
This channels are from UPC tubes and are connected to pulser PB-5.
We found that the threshold of external trigger was set to 1V
instead to 1.8V as before and this was producing a double pulse (see photo)
like triggering on the fall and rise of the trigger pulse.
This happen whenever the threshold as below 1.6V.
We do not understand this: the signal has +2.2V and no apparent ripple (!????).
We set threshold to 1.8V and now is OK |
Attachment 1: He121.png
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359
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Tue Oct 16 08:57:56 2018 |
ATD & JLT | 252Cf source |
252Cf source Run
START:?
STOP: 16:56
ROOT file: 181016_1656_252Cf.root |
Attachment 1: 181016_1656_252Cf.root
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358
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Tue Oct 16 03:15:03 2018 |
ATD & JLT | Start of REP run preparation (RIBF148) |
16-Oct-2018
- Start DACQ computer: OK!
- Create directory: /data/1810Preparation/
- Copy last configuration RIBF139 file: 171119_1126_Conf_BrikenFullYSO.xlsx
- Return PB-5 pulser into crate and set parameters
- Star all crates: OK!
- Start DACQ: OK!
- Rename configuration file and edit to eliminate YSO related parameters
New Config file: 181016_Conf_BrikenFull.xlsx
- Start 3He tube HV: power the ethernet hub, power the pixie PC,
edit the hvmon.conf file (only tubes active), run hvmon: OK!
- We realized that current and voltage of VME crate 1 was oscillating.
We pulled out V1A7 (not used) and it became stable: seems that we are at the limit of
power supply: OK!
- We put the 252Cf source in and check gain match:
only (the gain of) three tubes moved slightly since the last run (one year ago)!
He006, He134, He135 -> new calibration: OK!
- We move SIS3820 clock from internal to external frequency:
Setup UK Tektronix clock: 25MHz, square signal, 800mVpp, -400mV offset
Plug in Lupo module (VME1 crate): OK!
ISSUE: the current placement of the table supporting the MUSIC chamber
is too close to the VME1 crate and one of the modules (V1A4)
cannot be extracted in case of failure. However V1A7 is unused
in this run and can be used as replacement. |
Attachment 1: Screenshot_from_2018-10-16_14-57-33.png
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357
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Fri Dec 1 07:29:47 2017 |
Vi Ho Phong | [Hardware][Configuration] Return the PB-5 Pulse generator (Pulser 2) and the 428F Linear Fan in-out modules and replace with a new Linear Fan in-out module |
The PB-5 Pulse generator labeled "Pulser 2" and the 428F Linear Fan in-out labeled "Clover G7" from BRIKEN NIM crate have to be returned to the RIBF electronics pool because the
borrowing time is expired.
For the Pulser 2, the external trigger input and pulse output cables were labeled before removing the module.
- Attachment 1: Original position and cabling of the pulser. The serial number of the pulser is 052010010247
- Attachment 2: A picture of the crate after removing the pulser.
- Attachment 3: Original Pulser setting.
The Linear Fan in-out was replaced with a new module (same version 428F), which can be used for a long time. The position of the input and output cables in the module were kept
unchanged.
- Attachment 4: Original position and cabling of the Linear Fan in-out module. The serial number of the original module is 051999070282
- Attachment 5: New Linear Fan in-out module after replacement.
- Attachment 6: Oscilloscope view of the 10kHZ NIM test input signal (blue) and output signal (yellow) of the old Linear fan in-out module.
- Attachment 7: Oscilloscope view of the 10kHZ NIM test input signal (blue) and output signal (yellow) of the new Linear fan in-out module. |
Attachment 1: pulser_old_position_cables.JPG
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Attachment 2: pulser_new_position_cables.JPG
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Attachment 3: pulser_setting_crop.jpg
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Attachment 4: linear_faninout_old_position_cables.JPG
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Attachment 5: new_linear_faninout_cables.JPG
|
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Attachment 6: old_linear_faninouttest.JPG
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Attachment 7: new_linear_faninout_test.JPG
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356
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Fri Nov 24 00:45:36 2017 |
AT | ur17b BRIKEN files |
List of files in BRIKEN DAQ PC:
Experiment DA1702 (including the test with YSO during first night)
*.dlt: 350
*.xlsx: 10
*.root: 162
Experiment RIBF139
*.dlt: 162
*.xlsx: 7
*.root: 101 |
355
|
Thu Nov 16 02:32:23 2017 |
BRIKEN collaboration | YSO thresholds |
YSO Tests
Thresholds & calibrations
For HV between (500,600)V, the rate of visual scalers do not change. The current thresholds,
Ch Thr
xa 130
xb 130
ya 130
yb 150
dy 90
Attachment 1: dynVSdynGated.
>>Black, dyn signal
>>Red, dyn signal gated by 4 anodes (histo xpos) |
Attachment 1: dynVSdynGated.png
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354
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Tue Oct 31 06:57:53 2017 |
OH, TD | AIDA Oct17 Beam Test Analysis |
PDF file attached with the preliminary analysis of the October 2017 AIDA in beam test. |
Attachment 1: AIDA_Test_Results.pdf
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353
|
Fri Oct 27 10:04:31 2017 |
SG, RY | LISE++ file for BRIKEN1 |
Here attached the lise file for BRIKEN1 |
Attachment 1: Cu82_Be5mm_Brho7.7000Tm_F1deg8mm_F5deg8mm_F7_D80mod_F11
|
Version 10.0.27
{============================= Main Part ======================================}
[general]
File = C:\users\sgo\Desktop\Cu82_Be5mm_Brho7.7000Tm_F1deg8mm_F5deg8mm_F7_D80mod_F11
Date = 27-10-2017
Time = 17:57:52
Configuration = C:\Users\inabe\Desktop\laa.lcn
Optionsfile = A1900_2006.lopt
Title = BigRIPS Standard + ZDS Large Acceptance Achromatic mode
BlockStructure = DSSAWMSMDSAMMMMMASMMMMMMMMDMDMMAWSMMDMDMMMMMASMMMMMASMMMAMMDSMMMSSMMMDMMSMMAMMMMMMMMMMSMMMMMMMMSMMM
[settings]
A,Z,Q = 238U 86+ ; Mass ElementName Charge+ Beam
Energy = 345 MeV/u
Intensity = 50 pnA ; enA,pna,pps,kW
RF frequency = 20 MHz
Bunch length = 1 ns
Settings on A,Z = 82Cu ; Mass ElementName Charge+ Beam
[OpticsBeam]
BX = 0.5 (±)mm ; one-half the horisontal beam extent (x)
BT = 5 (±)mrad ; one-half the horisontal beam divergence(x')
BY = 0.5 (±)mm ; one-half the vertical beam extent (y)
BF = 5 (±)mrad ; one-half the vertical beam divergence (y')
BL = 30 (±)mm
BD = 0.1 (±)% ; one-half of the momentum spread (dp/p)
ShiftX = 0 mm ; beam respect to the spectrometer axis
AngleX = 0 mrad ; beam respect to the spectrometer axis
ShiftY = 0 mm ; beam respect to the spectrometer axis
AngleY = 0 mrad ; beam respect to the spectrometer axis
Scheme Angle = 60 degrees
ShapeX = 1
ShapeT = 1
ShapeY = 1
ShapeF = 1
ShapeL = 1
ShapeD = 1
OptBeam_X = 1 (±)mm
OptBeam_T = 30 (±)mrad
OptBeam_Y = 1 (±)mm
OptBeam_F = 30 (±)mrad
OptBeam_L = 0 (±)mm
OptBeam_D = 1.5 (±)%
[SlitsBeforeTarget]
Shape = 1 ; 0-slits, 1-ellipse
ApertureShape = 1 ; 0-slits, 1-ellipse
X_action = 0,0,0 ; Use 1/0, Show 1/0, UseApp 1/0
X_size = 1,-2.00,-50.0,2.00,50.0 ; joint,Left,L-limit,Right,R-limit
Y_action = 0,0,0 ; Use 1/0, Show 1/0, UseApp 1/0
Y_size = 1,-2.00,-50.0,2.00,50.0 ; joint,Bottom,B-limit,Top,T-limit
[options]
NP simple = 32 ; Number of points in distribution
NP charge states = 32 ; Number of points in distribution
NP wedge = 32 ; Number of points in distribution
Charge states = Yes ; No & Yes
CutEdgeEffect = 1 ; 1-Yes. Default, 0-no - for extended configurations
Prim.beam scatter = 0 ; 0-without, 1-with
Delta peak = 0 ; 0-without, 1-with
BrhoMeanMax = 0 ; 0-Max, 1-Mean
BrhoMeMaLeRi = 3 ; 0-Max, 1-Mean, 2-Left, 3-Right /for fission/
[target]
Target contents = 0,4,1,9.012 ; Nomer,Z,Atoms,Mass
Target thickness = 4,5,1.848,0,0 ; State,Thickness,density,angle,SolidGas
Target fusion compound = 0
Targ use for Q-states = 1
Target Defect = 1,0 ; [0] choice - % or micron at 0 degree, [1]=value;
Degrader contents = 0,6,1,12.011 ; Nomer,Z,Atoms,Mass
Degrader thickness = 0,0,2.26,0,0 ; State,Thickness,density,angle,SolidGas
Degra use for Q-states = 1
Degrader Defect = 1,0 ; [0] choice - % or micron at 0 degree, [1]=value;
[mechanism]
Reaction = 6 ; 0 - fragm, 1 - fusion-resid, 2 - fusion-fission
CalcOther = 112 ; calculate other reactions
V calculation = 3 ; 0 - constant, 1 - Borrel, 2 - Rami, 3-convolution, 4-two body reaction
V_opt/Vbeam = 1 ; default 1
Velocity_exceed = 1 ; 0 - without, 1-with - two-body recations velocity corrections
Binding Energy for Vf/Vp = 8 MeV ; Binding energy for Borrel's expression
Shift for Vf/Vp calc = 0
Prefragment_Rami = 1 ; 1-Yes, 0-No
Sigma0 = 90 MeV/c ; default 90
SigmaD = 200 MeV/c ; default 200
SigmaM = 87 MeV/c ; default 87
Asymmetry = 0 % ; default 0
Method v-sigma = 3 ; 0 - Goldhaber, 1-Morrissey,2-Friedman,3-Convolution
G_Surface = 0.95 MeV/fm^2
Symmetry around half_Ab = 1 ; 1 - yes, 0-no
Pfaff pickup correction = 1 ; 1 - yes, 0-no
ChargeExchangePfaff = 1 ; 1 - exclude, 0-forget
Sigma corr 0 = 0 ; Coulomb energy
Sigma corr 1 = 0 ; Projectile mass
Friedman mode = 2 ; 0-Qgg, 1-Surface, 2-Qgg+Surface
Prefragment_Fri = 1 ; 1-Yes, 0-No
Coulomb_Friedman = 1 ; 1-Yes, 0-No
K_Morr = 8 MeV/A ; E/A=8MeV/A default; D.Morrissey coef.
K_MorHalf = 8 MeV/A ; E/A=8MeV/A default at Afrag=Aproj/2; D.Morrissey coef.
AA_fast = 0 ; 1-Yes, 0-No
BarrierShape = 1 ; 0-classical, 1-quantum mech.
H_omega = 5 MeV ; default 3
Probabilty_CN = 1 ; 0/1 use Prbabilty for CN formation
UseVanishing = 1 ; 1-Yes, 0-No
VanishMode = 0 ; 0-Sierk, 1-Cohen
NuclPotential = 1 ; 0-Bass, 1-WS
WS_V0 = 105 MeV
WS_R0 = 1.12 fm
WS_a = 0.75 fm
FusDiffuseness = 1
Width Coef = 1 ; default 1; for Leon's charge state distribution
gZt Correction = 1 ; default 1; Leon's C.S.D.
PowerCoefLeon = 0.477 ; default 0.477; Leon's C.S.D.
Cross section = File ; Fit & File
Charge method = 3 ; charge calculations method 0-5
EPAX Cross Section = 4 ; cross section calculations method 0-4
SR Cross Section = 2 ; EPAX for SR 0-2
Energy Loss = 2 ; energy loss calculation method 0-3
Anglular straggling = 1 ; 0-LISE, 1-ATIMA
StragglingCoef1 = 0.217
StragglingCoef2 = 1.12
Energy straggling = 1 ; 0-LISE, 1-ATIMA
EnergyStragMethod = 0 ; 0-integrate, 1-table
EnergyStragShape = 0 ; 0-Gauss, 1-Landau-Vavilov
EquilThickness = 1 ; 0-Charge, 1-Global
MassMethod = 0 ; 0-DB+calcul, 1 + just calcul
MassDataBase = 0 ; 0-A&W, 1-User ME
Mass formula = 2 ; 0-LDM, 1-Myerer, 2: 1+corrections
UseChargeForEnergy = 2 ; 0-No, 1-Yes, 2-Auto
EnergyValueAuto = 30 ; default value 30 MeV/u
EquilibriumMode = 0 ; 0-Equil, 1-NonEquil
UB_Global = 70 ; default 70 MeV/u
MinZ_Global = 2 ; default Z>=29
ChargeStateOptim = 1 ; 0-No, 1-Yes
ZmQ_AfterReactn = 0 ; default 0 (full stripped)
EPAX_p_Norm = 1
EPAX_p_Un = 1.65
EPAX_p_Up0 = 1.79
EPAX_p_Up1 = 0.00472
EPAX_p_Up2 = -1.3e-5
EPAX_p_H = 1
[fission]
FisAngDistShape = 0 ; 0-isotropic; 1-anisotropic
FisMomCutForAngDist = 2 ; 0-dont use; 1-use just MatrixKinematics; 2-use for all; (default 2)
OddEvenCorrections = 1 ; 0-dont use; 1-use
PostScissionEvaporation = 1 ; 0-dont use; 1-use
DeexcitFunctionPoints = 0 ; 0- average deexcitation energy; 1- 3 points; 2 - manually
FisEXmanually = 20 ; Excitation energy manually
FisCSmanually = 1000 ; Cross section manually
FisTXEmethod = 1 ; 0-from Edissipated, 1 from Q-value
Fis_f = 0.0045 ; default 0.0045
FisEXsigma = 5.5 MeV ; default 5.5
FisCS_Global = 1e-15
FisCS_TKE = 1e-8
N0 = 83 ; default 82
dU0 = -2.65 ; default -2.5
C0 = 0.7 ; default 1.4
cpol0 = 0.65 ; default 0.65
width0 = 0.63 ; default 0.63
N1 = 90 ; default 90
dU1 = -3.8 ; default -5.5
C1 = 0.15 ; default 0.16
cpol1 = 0.55 ; default 0.55
width1 = 0.97 ; default 0.97
[charge_suppression]
FragInd = 1e-3
FragTotal = 1e-5
BeamInd = 1e-9
BeamTotal = 1e-11
[convolution]
Convolution mode = 2 ; 0-Qgg, 1-Surface, 2-Qgg+Surface
SigmaConv = 91.5 MeV/c ; default 90 for Convolution
CoefConv_0 = 3.344
CoefConv_1 = 5.758
CoefConv_2 = 2.936
ShiftConv_0 = 0.158
ShiftConv_1 = 0.149
ShiftConv_2 = 0.153
[evaporation]
NP evaporation = 16 ; Number of points in distribution
EvapMethod = 2
StateDensityMode = 2 ; 0, 1+pairing, 2+shell
EvapUnstableNuclei = 1 ; 0 - only stable,1 +unstable
Tunnelling = 1 ; 1-Yes, 0-No
AvoidUnboundCS = 1 ; 1-Yes, 0-No
ProtectedChannels = 1 ; 1-Yes, 0-No
R_Evaporation = 5.7 fm ; correction for the effective Coulomb barrier
Mode_Apf_manual = 0 ; 1-manual, 0-auto
Energy_in_T = 2 ; default 2
EvaporationVelocity = 0 ; 0 - quality, 1 -fast
DeltaOddEvenEvap = 12
DeltaOddEvenFission = 14
BreakupTemperature250 = 4.7
BreakupTemperature150 = 5.9
BreakupTemperature050 = 8
BreakupDiffuseness = 0.05
DissipationKramers = 0 ; 0 - no, 1 - use
DissipationStepFunction = 1 ; 0 - no, 1 - use
DissipationBeta = 1 ; default 2.0
mode_1n = 1 ; 1-Yes, 0-No
mode_2n = 1 ; 1-Yes, 0-No
mode_1p = 1 ; 1-Yes, 0-No
mode_2p = 0 ; 1-Yes, 0-No
mode_a = 1 ; 1-Yes, 0-No
mode_d = 0 ; 1-Yes, 0-No
mode_t = 0 ; 1-Yes, 0-No
mode_3he = 0 ; 1-Yes, 0-No
mode_fis = 1 ; 1-Yes, 0-No
mode_brk_up = 1 ; 1-Yes, 0-No
mode_gamma = 0 ; 1-Yes, 0-No
[fission_barrier]
FissionBarrierFactor = 1
FissionBarrierMode = 1 ; #0-4
OddEvenCorrections = 1 ; 1-Yes, 0-No
ShellCorrections = 1 ; 1-Yes, 0-No
FB_InOutMax = 2 ; #0-2 - in/out/max
ModeForUser = 1 ; #0-2
NdeltaOddEven = 2.5
ZdeltaOddEven = 9
[excitation_energy]
GeomAA_Correction = 0 ; 0 - don't use,1 - use -default
Thermalization = 0 ; 1-Yes, 0-No
ThermaTimeCoef = 3e-22 ; 2.1e-22 MeV *s/e(t)
Friction = 0 ; 0 - off,1 - on
Ev_A_SigmaCoef = 9.6
G_FrictionCoef1 = 6.5
G_FrictionCoef2 = 0
G_FactorCoef1 = 1.5
G_FactorCoef2 = 2.5
DepthHole = 40
EnergyCoef_CB0 = 0
EnergyCoef_CB1 = 13.3
EnergyCoef_CB2 = 0
SigmaCoef_CB0 = 0
SigmaCoef_CB1 = 9.6
SigmaCoef_CB2 = 0
D_MeanTemp = 13
[evapauto]
tun_a0 = 1.00938
tun_a1 = -0.36149
tun_a2 = 0.21551
A_Bound = 300 ; mass
A_Pairing = 12 ; mass
[plot]
Start target = Detector ; Detector & RF
Start of TOF = M8
Stop of TOF = M28
dE-detector-1st = M24
dE-detector-2nd = M28
TKE-detector = M17
PlotBrho = D1
PlotWedge = S4
X-detector = M17
Y-detector = M17
Tilting = M1
Stopper = M2
RO_Wedge = n
ConditionBlock = A10
Plot threshold = 1e-10 pps ; minimal value for plot scale
Shift of TOF for RF = 0 ns ; for dE-TOF plot with RF
Fraction of RF trigger = 1
UseCondition = 0
TKE_calibration = 1,1,0,MeV ; Input PV(0) or CH(1), A, B, dimension
[cs_file]
UserDiffCS = 0 ; Number of User Diff CS saved in this file
AppendOverwrite = 0
AttachedInside = 1
ShowCSinPlot = 1
Chi2 = 1
CSfilename = \\Mac\Home\Desktop\BRIKEN\CrossSections\xsec_g4top_settin1_lise.cs
[sec_reactions]
NP sec.reactions = 16 ; Number of points in distribution
Secondary reactions = 0 ; 0/1 - use secondary reactions in calculations
fiss_FilterUse0 = 0
fiss_FilterUse1 = 0
fiss_FilterUse2 = 0
fiss_ellipse = 5
fiss_NdeltaTop = 0
fiss_ZdeltaTop = 0
fiss_NdeltaBot = 25
fiss_ZdeltaBot = 20
frag_FilterUse0 = 3
frag_FilterUse1 = 3
frag_FilterUse2 = 3
frag_ellipse = 4
frag_NdeltaTop = 5
frag_ZdeltaTop = 5
frag_NdeltaBot = 6
frag_ZdeltaBot = 6
... 5150 more lines ...
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Attachment 2: nuclei.png
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352
|
Thu Oct 26 09:01:53 2017 |
BCR | Number of Counts vs Expected Efficiency for Proposals |
Here is a doc with an estimate of the statistical uncertainty P1n and P2n as a function of the number of implant-beta correlations for future experiments.
This will hopefully be useful for the new PAC proposals as an estimate for the time needed to measure a certain precision.
If there are any questions please feel free to email me (Charlie Rasco).
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Attachment 1: ExpectedBRIKEN_Precision.pdf
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351
|
Wed Oct 25 19:14:09 2017 |
NB | First pass efficiency for current experiment |
I roughly (~10%) checked the efficiency for 4 of the peaks from 171025_1222_1355_152EuCloverCal.root.
I checked the peaks at 122, 245, 344, and 1408. The indication is an efficiency of 6.9, 9, 9,8, and 2.6 % for these gamma rays repectively.
Previously the efficiency was 11.1, 7.1, 5.3, and 1.6% . This indicates a reduction in efficiency below ~200 keV (because of YSO) and otherwise there is an increase in efficiency from 40% at 245 keV and up to 65% at 1480 keV.
A more complete analysis will come later.
|
350
|
Wed Oct 25 18:12:43 2017 |
Sunflower collaboration | Gamma sources web page |
http://www.nishina.riken.jp/collaboration/SUNFLOWER/misc/util/ribfsource.html |
349
|
Wed Oct 25 17:49:09 2017 |
JT, AM, NB, DS, DM, AT | pulser in CLOVERS |
G7 pulser weird behavior
Pulser signals G7Red & G7Green were crossed before the digitizer (the aluminium potato?)
Pulser removed from G7Red & G7Green
Background measurement
Start: 01:44
Run: 000
File: 171026_0144_bck_000.dlt
Stop: |
348
|
Wed Oct 25 01:02:14 2017 |
RG | Status of the YSO array |
The presently used detector has 48x48x5 mm3 YSO array with 1x1mm2 segments. They are separated with ESR. We use H8500 pspmt and 2 mm quartz diffuser with rough edges. Coupling is done with sylgard. Anger logic uses a conventional resistive network with 1kohm and we have 4 position signals and dynode. The position signals (xa,xb,ya,yb) are split in Low gain branch connected directly to 5V range input in Struck and High gain branch, which uses Phillips fast amplifier to boost the gain. The use of the amplifiers enables to operate the detector at low PSPMT gain and should give us a chance to work with the strong light produced by the implant. The implant signals were simulated using blue diode and a pulse generator. We observed significant drift of the position for very large pulses, but this was for now attributed to be the pulse shape effect due to the use of the diode and reltively slow pulser.
YSO for now should run at -700 V. The maximum operating voltage is 1200V and should not be exceeded. At 1200 V the ions induced signals may saturate our electronics.
Tuesday evening:
Detector remounted in the pedestal and aligned with WASABI with 1mm+1.5mm spacers. The pedestal is 25.8 mm tall and the box is 60 mm tall. We checked also the orientation of the spectra and chose AIDA convention (look upstream). With this pedestal the front of the box is centered with the back of the clover leaf.
Wednestay morning:
I opened the detector and rewrapped it with new teflon tape. I noticed a small piece if sylgard peeled off, which may explain why the we had some edge effect yesterday. The detector was remounted on the new pedestal which will allow it to be positioned at the center of the clover. The signals looked OK on the oscilloscope.
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347
|
Tue Oct 24 13:14:47 2017 |
RY | Calibration data for clovers |
for energy calibration with 152Eu source
171024_1858_152Eu_G7.root
171024_2112_152Eu_D4.root |
Attachment 1: 171024_1858_152Eu_G7.root
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Attachment 2: 171024_2112_152Eu_D4.root
|
346
|
Tue Oct 24 03:08:23 2017 |
RG, RY, MS, JA, RCF, SG, AT | light pulser YSO |
light pulser measurement
SN's pulse generator 20ns width |
Attachment 1: 171024_1107_YSOPlots.root
|
Attachment 2: Screenshot_from_2017-10-24_11-09-54.png
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|
345
|
Mon Oct 23 09:43:00 2017 |
RG, RY, MS, SG, AT | 137Cs YSO |
measurement of 137Cs with YSO
after matching the gains of the
HighGain channels
YSO detector was inside the black box, outside the matrix.
The source was placed in front of the YSO
First measurement
Start: 15:14
End: 16:55
RootFile: 171023_1655_137CsYSO.root
Second measurement (same conditions )
Start: 16:55
Run number: 070
End: 17:41
File: 171023_1655_137CsYSO_070.dlt
RootFile: 171023_1655_1741_137CsYSO_070.root
The 137Cs source is weak; the rate of the YSO detector was about 50Hz (without source is 10Hz). |
Attachment 1: 171023_1655_137CsYSO.root
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Attachment 2: 171023_1655_1741_137CsYSO_070.root
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Attachment 3: Screenshot_from_2017-10-23_17-51-37.png
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Attachment 4: Screenshot_from_2017-10-23_17-54-53.png
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|
344
|
Sun Oct 22 11:32:59 2017 |
JA,ATD, JLT | New Gasific Configuration file |
|
Attachment 1: 171022_1846_Conf_BrikenFullYSO.xlsx
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343
|
Sun Oct 22 11:14:35 2017 |
JA,ATD,JLT,RG,RY,SG,MS,PV,Liu,KR | 252Cf source Wasabi-BrikenYSO |
252Cf source in the middle of Wasabi and YSO in front of Clover D4
Start: 19:15
BRIKEN File: 171022_1915_252Cf_BrikenYSO_068.dlt
Wasabi File: prerun0029.evt
Stop: 19:24
BRIKEN File: 171022_1915_252Cf_BrikenYSO_069.dlt
Wasabi File: prerun0034.evt
Online file: 171022_1915_1924_252Cf_BrikenYSO.root |
342
|
Sun Oct 22 10:26:44 2017 |
JA,ATD,JLT,RG,RY,SG,MS,PV,Liu,KR | First Wasabi-YSO-BRIKEN correlation test |
60Co source between YSO and Wasabi in front of D4 Clover
Briken configuration file: 171022_1811_Conf_BrikenFullYSO.xlsx WRONG!!!
Start: 18:25
BRIKEN File: 171022_1825_60Co_BrikenYSO_040.dlt
Wasabi File: prerun0007.evt
Stop: 18:37
BRIKEN File: 171022_1825_60Co_BrikenYSO_066.dlt
Wasabi File:prerun0007.evt
Hughe amount of data!?:
Ch1-4 have 100 samples/event
Ch1 Samples MAW was activated
Ch5-8 have TriggerGateLength=10000samples & 10000 samples/event
We make a new measurement:
New Configuration file: 171022_1846_Conf_BrikenFullYSO.xlsx
Start: 18:57
Briken file: 171022_1856_60Co_BrikenYSO_067.dlt
Wasabi File: prerun0022.evt
Stop:19:06
Briken file: 171022_1856_60Co_BrikenYSO_067.dlt
Wasabi File: prerun0027.evt
Root file: 171022_1857_1906_60Co_BikenYSO.root |
Attachment 1: 171022_1846_Conf_BrikenFullYSO.xlsx
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Attachment 2: 171022_1846_60Co_WasabiBrikenYSO.png
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|
341
|
Sun Oct 22 08:52:17 2017 |
KR,JA,ATD,JLT | Clover resolution |
Resolution check using 40K 1460 keV line
in the background measurement overnight
(File: 171022_0126_1101_bck.root)
D4: 2.9 1keV @ 1461.8 keV
G7: 2.98 keV @ 1460.0 keV |
340
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Sun Oct 22 05:15:26 2017 |
RG,RY,MS,ATD,JA,JLT | Check of YSO |
We start a systematic check of YSO in BRIKEN DACQ
WE check and correct a configuration file for YSO alone
Conf file: 171022_1306_YSO_Conf.xlsx
First measurement:
change the light pulser attenuation and check
changes of X and Y position
Root file: 171022_1314_pulserAtCenter.root
We change configuration file to remove amplitude
range condition to buil position
New configuration file:171022_1332_YSO_Conf.xlsx
Now start moving the light pulser position using a mask:
Light pulse position: Top Left Out
Root file: 171022_1335_pulseTopLeftOut.root
Light pulse position: Bottom Left Out
Root file: 171022_1341_pulseBottomLeftOut.root
Light pulse position: Bottom Right Out
Root file: 171022_1345_pulseBottomRightOut.root
Light pulse position: Top Right Out
Root file:171022_1350_pulseTopRightOut.root
Light pulse position: Top Left In
Root file: 171022_1401_pulseTopLetIn.root
Light pulse position: Bottom Left In
Root file: 171022_1406_pulseBottomLeftIn.root
Light pulse position: Bottom Right In
Root file: 171022_1410_pulseBottomRightIn.root
Light pulse position: Top Right In
Root file: 171022_1416_pulseTopRightIn.root
Now we ramp the PMT high voltage starting at 600V:
600V, 650V, 700V, 750V, 800V, 900V, 950V, 1000V, 1050V, 1100V, 1150V
Pulser at Top Left Out
Root file: 171022_1445_HVramp_pulseTopLeftOut.root |
Attachment 1: 171022_1306_YSO_Conf.xlsx
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Attachment 2: 171022_1314_pulserAtCenter.root
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Attachment 3: 171022_1332_YSO_Conf.xlsx
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Attachment 4: 171022_1335_pulseTopLeftOut.root
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Attachment 5: 171022_1341_pulseBottomLeftOut.root
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Attachment 6: 171022_1345_pulseBottomRightOut.root
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Attachment 7: 171022_1350_pulseTopRightOut.root
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Attachment 8: 171022_1401_pulseTopLetIn.root
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Attachment 9: 171022_1406_pulseBottomLeftIn.root
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Attachment 10: 171022_1410_pulseBottomRightIn.root
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Attachment 11: 171022_1416_pulseTopRightIn.root
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Attachment 12: 171022_1445_HVramp_pulseTopLeftOut.root
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339
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Sat Oct 21 17:30:23 2017 |
JA, ATD, JLT | Background measurement overnight |
22/10/2017
Start: 01:26
Run: 037
Stop: 11:01
Run: 039
List mode: 171022_0126_bck_*.dlt
Root file: 171022_0126_1101_bck.root
Observations:
1. The noise in 3He tubes has been effectively suppresed
(compare figure of BRIKEN spectrum in attachment with similar
figures of previous runs)
2. The 252 Cf source used immediately before has activated
something as can be deduced from the change of rate
in the D4 detector compared to G7 (standing on the floor)
see picture below. The effective half-life of the activation is
T1/2=71.8min
(see figures in attachment) |
Attachment 1: Screenshot_from_2017-10-22_11-26-49.png
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Attachment 2: Screenshot_from_2017-10-22_11-26-10.png
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Attachment 3: Screenshot_from_2017-10-22_11-26-28.png
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338
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Sat Oct 21 17:14:55 2017 |
JA, ATD, JLT | 252Cf efficiency calibration |
Measurement of BRIKEN neutron counter efficiency
252Cf source in the (approximately) center
Wasabi and D4 clover inserted. G7 on the floor.
YSO on the box with light pulser.
The source was plug in a Styrofoam piece at the right height
so that it could be centered longitudinally with the D4 Clover
and transversely with the Wasabi nose.
Possible position difference with previous efficiency
measurements using the cardboard source holder
should not impact the efficiency obtained.
Start: 00:41
Stop: 01:08
Run number: 36
List mode: 171022_0041_252Cf_036.dlt
Root file: 171022_0041_0108_252Cf.root
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Attachment 1: Screenshot_from_2017-10-22_01-21-51.png
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337
|
Sat Oct 21 17:11:03 2017 |
JA, ATD, JLT | New Gasific configuration file |
Configuration file saved on 22-Oct-2017 at 00:59
after increasing all the threshold in all 3He tubes to about 100keV.
Also the threshold of Clover detectors was slightly increased. |
Attachment 1: 171022_Conf_BrikenFullYSO.xlsx
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336
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Sat Oct 21 17:05:21 2017 |
JA,ATD, JLT | New DACQ hardware configuration |
Configuration of BRIKEN DACQ hardware:
Detector->VME->ADC->Channel
New configuration:
Ancillaries are moved to crate #2: V2A8 (SIS3316)
YSO is on crate #1: V1A7 (SIS3316)
V2A4 (SIS3302) failed and was replaced wit spare unit (Chan #5 missing)
Ancillaries are reduced to F11 Plastic (Right and Left, Direct and Attenuated)
and AIDA Plastic veto. The 10Hz pulser signal is also fed to this ADC (Dead Time Pulser).
YSO provides 5 signals: xa, xb, ya, yb and dynode.
Each signal is splitted. One branch of xa,xb,ya,yb is amplified
the other goes directly (but it might be eventually attenuated).
See attached file |
Attachment 1: TubeAncillaryDACQDistribution-October2017.xlsx
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335
|
Sat Oct 21 07:26:13 2017 |
NB, RY, BD, MS | Corrected Calibration D4 |
K R G B
m 0.001558636 0.0006599344 0.0015311753 0.0015807021
b -0.6545742444 0.4330534066 2.001278013 1.0994163913
FWHM are <= 3 keV @ 1408
K R G B
3.1458290692 2.5879235958 2.9829238667 3.0707781948
The green leaf of D4 may have a noticeable non-linearity above 1MeV. |
Attachment 1: D4Oct19.ods
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334
|
Sat Oct 21 04:18:17 2017 |
NB | Draft of Instructions for HV |
Setup:
2 MPOD + cards with 8 channels each one where the 10 BRIKEN PA are connected.
1 MPOD + card with 8 possible inputs where the 8 Ge are powered
1 MPOD – card with YSO detector
The visualiser located in the local IP accessible webpage 192.168.13.239 must show the implemented changes. Open webpage first!
Pre-Amplifier HV Card Card Channel Voltage 3He Tubes
PA1 (diff) 1 0 1450 VRIKEN: Ø 2.54cm (5.132 atm)Download specifications (Downstream counters)
PA2 (diff) 1 1 1450 VRIKEN: Ø 2.54cm (5.132 atm)(Upsteram counters)
PA3 (diff) 1 2 1550 VUPC: Ø 2.54cm (8atm)
PA4 (diff) 1 3 1550 VUPC: Ø 2.54cm (8atm)
PA5 (single) 1 4 1550 VUPC: Ø 2.54cm (8atm)
PA6 (single) 2 100 1200 VORNL: Ø 2.54cm (10.26atm)Download specifications
PA7 (single) 2 101 1750 VORNL: Ø 5.08cm (10.17atm)Download specifications
PA8 (single) 2 102 1750 VORNL: Ø 5.08cm (10.17atm)
PA9 (single) 2 103 1750 VORNL: Ø 5.08cm (10.17atm)
PA10 (single) 2 104 1750 VORNL:Ø 5.08cm (10.17atm)
High voltage control: All High voltage 3He and HPGe can now be set via a configuration file called hvmon.conf and a program called hvmon. hvmon also watches the temperature of the HPGe via the RTD outputs and sets trip and other safety settings.
The important locations are as follows:
-
Path for conf file: /home/pixie16/DAQ_BRIKEN/include/hvmon.conf
-
Path for temperature monitor: /home/pixie16/DAQ_BRIKEN/kelvin/kelvin-u3
-
Path for temperature logging: /home/pixie16/DAQ_BRIKEN/kelvin/kelvin-log
-
Path for temperature log control: /home/pixie16/DAQ_BRIKEN/kelvin/kelvin-read
-
Path for hvmon: /home/pixie16/DAQ_BRIKEN/hv-mpod/hvmon
-
Path for hvmon control: /home/pixie16/DAQ_BRIKEN/hv-mpod/hvmon-read
This is also the order in which the programs should be run at first.
If the kelvin temperature monitoring programs are already running ('ps -A | grep kelvin' to check) and you wish to change the settings:
-
Adjust hvmon.conf
-
stop 'hvmon' with ctrl+c
-
rerun by './hvmon' (also 'up + Enter')
If kelvin is not running, in a separate window or screen
-
cd /home/pixie16/DAQ_BRIKEN/kelvin/
-
./kelvin-u3 &
-
./kelvin-log &
Then proceed with the above.
This is also the order in which the programs should be run at first.
If the kelvin programs are already running ('ps -A | grep kelvin' to check) and you wish to change the settings:
2 OPTIONS!
Option 1:
Adjust channels that have previously been declared by using
./hvmon-read
16
and follow on screen instructions. If channels have not been declared previously in hvmon.conf → proceed to option 2.
Option 2:
-
Adjust hvmon.conf
-
stop 'hvmon' with ctrl+c or by ‘100’ at hvmon-read
-
rerun by './hvmon &' (also 'up + Enter')
The example below turns on ALL detectors PA (Pre-amps1-10), D4/G7 HPGe (KRGB, Black, Red, Green, Blue), and YSO/Gari. This example sets all detectors voltage,ramp up/down speed and status (0/1 = Off/On respectively). IMPORTANT! Ramp speed goes card by card.
UPDATE!!
3He Preamps now run up and down by a small ramp for the first 50V hardcoded into hvmon via the ‘PA’ keyword. This avoids the reset fault.
EXAMPLE hvmon.conf:
Type IP address channel slot name voltage Current RampUp RampDn Switch On/Off
V A V/s V/s 1/0
------ --------------- --------- ----- ---- ------- ------- ------ ------ -------------
0 192.168.13.239 0 0 PA1 1450 0.0001 50 50 1
0 192.168.13.239 1 0 PA2 1450 0.0001 50 50 1
0 192.168.13.239 2 0 PA3 1550 0.0001 50 50 1
0 192.168.13.239 3 0 PA4 1550 0.0001 50 50 1
0 192.168.13.239 4 0 PA5 1550 0.0001 50 50 1
0 192.168.13.239 5 0 OFF 0 0.0001 50 50 0
0 192.168.13.239 6 0 OFF 0 0.0001 50 50 0
0 192.168.13.239 7 0 OFF 0 0.0001 50 50 0
0 192.168.13.239 0 1 PA6 1200 0.0001 50 50 1
0 192.168.13.239 1 1 PA7 1750 0.0001 50 50 1
0 192.168.13.239 2 1 PA8 1750 0.0001 50 50 1
0 192.168.13.239 3 1 PA9 1750 0.0001 50 50 1
0 192.168.13.239 4 1 PA10 1750 0.0001 50 50 1
0 192.168.13.239 5 1 OFF 0 0.0001 50 50 0
0 192.168.13.239 6 1 OFF 0 0.0001 50 50 0
0 192.168.13.239 7 1 OFF 0 0.0001 50 50 0
0 192.168.13.239 2 2 YSO 700 0.0005 50 50 1
0 192.168.13.239 0 3 D40 3000 0.0001 5 5 1
0 192.168.13.239 1 3 D41 3000 0.0001 5 5 1
0 192.168.13.239 2 3 D42 3000 0.0001 5 5 1
0 192.168.13.239 3 3 D43 3000 0.0001 5 5 1
0 192.168.13.239 4 3 G70 2500 0.0001 5 5 1
0 192.168.13.239 6 3 G72 2500 0.0001 5 5 1
0 192.168.13.239 7 3 G73 2500 0.0001 5 5 1
-1
=================================================
Everything below type = -1 is treated as a comment
type = 0 => MPOD HV modules => accessed thru snmp
type = 1 => CAEN x527 HV modules => accessed thru CAENHVwrapper
With MPOD one can use IP address and channel numbers based on slot occupation
PA(1-4) are differential and PA(5-10) are unipolar.
In the program hvmon-read ‘Off’ always means ramp down and then turn off. The PA's like to hold on to voltage (~10-50V) and may cause a fault at ramp down and need reset. This should be Fixed with two stage ramping.
Warning!!: It has also been realized that mpod changes ramp up to be equal to ramp down. These parameters can be made equal for transparency.
To reset after fault use:
./hvmon-read
18 (or 5 then 18)
In case of power loss or other failure hit to do an emergency shutdown of the voltages.
./hvmon-read
5
Otherwise the Menu is as follows:
---------------------------------------------------------------------------------------
Global | Channels | Status
---------------------------------------------------------------------------------------
1 - Status | 11 - Clone channel |
2 - Force read | 12 - |
3 - Force read Temps | 13 - |
4 - All HV on | 14 - |
5 - All HV off | 15 - |
6 - Save conf file | 16 - Alter parameters |
7 - | 17 - Read from file |
8 - On list | 18 - Reset All Status' |
9 - Off list | 19 - Print Configure |
---------------------------------------------------------------------------------------
Time up - s
---------------------------------------------------------------------------------------
Temps (0,1,2) =(C,K,F):

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333
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Fri Oct 20 08:27:05 2017 |
BC Rasco | Analysis Slides |
Here are the ORNL/UTK BRIKEN analysis slides presented by BC Rasco on 2017/10/20.
Enjoy the fine reading.
The online seems to be missing some slides, but the pdf has all of the slides. |
Attachment 1: PreliminaryPnCalcsWithBkgCoin_BRIKENGroup.pdf
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332
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Fri Oct 20 05:33:11 2017 |
KR, NB, SG, RY, JL, AT: | Calibration and Resolution of D4 (after Repair) |
Green and Red channels were repaired by crimping and securing the grounding of the cables and fixing the cables securely to the table.
All problems during the repair process were visible on the scope. See example attatched.
Calibration is as:
Edit(10-21): NB realized calibration was not performed on the raw spectra, but on the previously calibrated ones. These values are wrong!
|
Red |
Green |
Blue |
Black |
m |
0.427423220774017 |
0.998884435913729 |
2.37782285204219 |
0.98418344391708 |
b |
0.530526265762205 |
0.578623397588558 |
0.699629095743376 |
-0.148161787849403 |
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Calculation also attached
FWHM (keV) @ 1408 values were:
Num Col FWHM (now) FWHM (before @ 1333)
G7 Red 3.06 2.77
G7 Green 2.81 2.84
G7 Blue 2.93 2.67
G7 Black 2.88 2.64
D4 Red 2.61 3.41
D4 Green 2.79 3.35
D4 Blue 2.88 3.60
D4 Black 3.17 4.85
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Attachment 1: IMG_20171019_105549066.jpg
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Attachment 2: D4Oct19.ods
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331
|
Wed Oct 18 08:46:23 2017 |
NB, SG, AT, JL | Clover G7 resolution |
G7 clover was on the stand
Source: 152Eu
File: 171018_1627_152Eu_G7.root
Resolution check for 1408 keV peak
FWHM(keV) Mean (keV)
G7Black 2.88 1407.2
G7 Red 3.06 1406.8
G7 Green 2.81 1407.0
G7 Blue 2.93 1406.5 |
Attachment 1: 171018_1627_152Eu_G7.root
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330
|
Mon Oct 16 05:52:14 2017 |
BRIKEN collaboration | START preparation |
We start to check every thing for the coming run
New directory: /data/1710Preparation/
Copy last configuration file of RIBF148 experiment
renamed:171016_Conf_BrikenFull.xlsx
Edinburgh clock parameters:
-Square signal.
-Amplitude: 1 Vpp
-Offset: 0.5V
-FreqCh1=FreqCh2
Status:
-F11 (high/low gain), AIDA_PL, DT_Pulser, Sync_Pulse, He tubes are defined and connected. Preliminary
configuration "171016_Conf_BrikenFull.xlsx" attached.
-YSO & clovers are not connected yet. |
Attachment 1: 171016_Conf_BrikenFull.xlsx
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329
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Thu Jun 15 10:07:56 2017 |
BRIKEN collaboration | Gamma calibrations |
Clover calibrations.
- Datafiles are located in the dac computer, path:
/data/1706FinalCalibrations/GammaCalibration
MEASUREMENTS
Configuration file: 170615_Conf_BrikenFull_AfterCrisis.xlsx
1) 152Eu. Source at the center of the moderator (0,0,0)
Source ID: 09 7011
Files: 170615_1805_152Eu_SourceNum272_000.dlt 170615_1805_1818_152Eu_SourceNum272.root
2) 137Cs. Source at the center of the moderator (0,0,0)
Source ID: 4763
Files: 170615_1837_137Cs_SourceNum4763_001.dlt 170615_1837_1846_137Cs_SourceNum4763.root
3) 152Eu. Source at the center of the moderator (0,0,0)????
Measurement over night.
Source ID: 09 7011
Files: 170615_1805_1850_152Eu_SourceNum272_002.dlt |
Attachment 1: WhatsApp_Image_2017-06-15_at_18.00.36.jpeg
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Attachment 2: WhatsApp_Image_2017-06-15_at_18.00.51.jpeg
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Attachment 3: WhatsApp_Image_2017-06-15_at_18.37.12.jpeg
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328
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Thu Jun 15 03:40:17 2017 |
BRIKEN collaboration | Z-scaning 252Cf Jun17 |
A scaning with 252Cf along the Z-axis of the neutron detector is carried out. The setup is similar to the scaning carried out in October 2016.
Observations:
- Clovers are put inside the detector without voltage.
- AIDA detector is out of the moderator.
- Position in Z is given with respect to the moderator side opposite to AIDA.
- The shielding for in-beam neutrons is mounted. It corresponds to HDPE 2.5cm + 1mm Cd + 20cm HDPE. The distance moderator to shieldind is 34.6mm
- There are two additional neutron sources in the Hall, aprox 10m from the detector. One 241AmBe (30mC) and 244Cm/O13 (500mC). Both sources produce an increase of the neutron background up to approx1n/s (x10 higher).
- Datafiles are located in the dac computer, path:
/data/1706FinalCalibrations/170615_Zscanning
MEASUREMENTS
Configuration file: 170615_Conf_BrikenFull_AfterCrisis.xlsx
0) A background measurement is carried out previous to the Zscan.
FILE: 170615_1100_Bkg.root
1) Z=25mm; Start 11:13 Stop 11:23
FILES: 170615_1113_Zscan_252Cf_25mm_000.dlt, 170615_1113_1123_Zscan_252Cf_25mm.root
2) Z=50mm; Start 11:25 Stop 11:34
FILES: 170615_1125_Zscan_252Cf_50mm_001.dlt, 170615_11125_1134_Zscan_252Cf_50mm.root
3) Z=75mm; Start 11:37 Stop 11:46
FILES: 170615_1137_Zscan_252Cf_75mm_002.dlt, 170615_1137_1146_Zscan_252Cf_75mm.root
4) Z=100mm; Start 13:25 Stop 13:33
FILES: 170615_1325_Zscan_252Cf_100mm_003.dlt 170615_1325_1333_Zscan_252Cf_100mm.root
5) Z=125mm; Start 13:36 Stop 13:44
FILES: 170615_1335_Zscan_252Cf_125mm_004.dlt 170615_1335_1344_Zscan_252Cf_125mm.root
6) Z=150mm; Start 13:51 Stop 13:59
FILES: 170615_1351_Zscan_252Cf_150mm_005.dlt 170615_1351_1359_Zscan_252Cf_150mm.root
7) Z=175mm; Start 14:01 Stop 14:09
FILES: 170615_1401_Zscan_252Cf_175mm_006.dlt 170615_1401_1409_Zscan_252Cf_175mm.root
8) Z=200mm; Start 14:12 Stop 14:21
FILES: 170615_1412_Zscan_252Cf_200mm_007.dlt 170615_1412_1421_Zscan_252Cf_200mm.root
9) Z=225mm; Start 14:24 Stop 14:31
FILES: 170615_1424_Zscan_252Cf_225mm_008.dlt 170615_1424_1431_Zscan_252Cf_225mm.root
10) Z=250mm; Start 14:33 Stop 14:40
FILES: 170615_1433_Zscan_252Cf_250mm_009.dlt 170615_1433_1440_Zscan_252Cf_250mm.root
11) Z=275mm; Start 14:43 Stop 14:50
FILES: 170615_1443_Zscan_252Cf_275mm_010.dlt 170615_1443_1450_Zscan_252Cf_275mm.root
12) Z=300mm; Start 14:54 Stop 15:01
FILES: 170615_1454_Zscan_252Cf_300mm_011.dlt 170615_1454_1501_Zscan_252Cf_300mm.root
13) Z=325mm; Start 15:04 Stop 15:11
FILES: 170615_1504_Zscan_252Cf_325mm_012.dlt 170615_1504_1511_Zscan_252Cf_325mm.root
14) Z=350mm; Start 15:14 Stop 15:22
FILES: 170615_1514_Zscan_252Cf_350mm_013.dlt 170615_1514_1522_Zscan_252Cf_350mm.root
15) Z=375mm; Start 15:24 Stop 15:31
FILES: 170615_1524_Zscan_252Cf_375mm_014.dlt 170615_1524_1531_Zscan_252Cf_375mm.root
16) Z=400mm; Start 15:34 Stop 15:41
FILES: 170615_1533_Zscan_252Cf_400mm_015.dlt 170615_1533_1541_Zscan_252Cf_400mm.root
17) Z=425mm; Start 15:44 Stop 15:57
FILES: 170615_1543_Zscan_252Cf_425mm_016.dlt 170615_1543_1557_Zscan_252Cf_425mm.root
18) Z=450mm; Start 15:59 Stop 16:08
FILES: 170615_1559_Zscan_252Cf_450mm_017.dlt 170615_1559_Zscan_252Cf_450mm_017.dlt |
Attachment 1: WhatsApp_Image_2017-06-15_at_18.11.52.jpeg
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327
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Wed Jun 14 06:22:21 2017 |
Ariel, Liu, Go, Nishinmura | HV is off |
To protect HPGe and 3He tubes from high intentsity primary beam, HV of these detector are off and the HPGe will be dismounted. |
326
|
Tue Jun 13 08:02:35 2017 |
briken team | 133Ba calibration |
After experiment 133Ba calibration
Working directory: /data/1706FinalCalibrations
Configuration file: 170604_Conf_BrikenFull_AfterCrisis.xlsx
DLT file name: 170613_1601_133Ba_002.dlt
Start: 16:02
Stop: 12:25 (2017/06/14)
Online rootfile: 133Ba_cal_z0_1602_1227nextday_170613.root
COMMENTS:
1. Source centered in both BRIKEN and clovers (faced towards clover D4)
2. No AIDA in
3. D4 clover pulsers are at 253, 260, 265, and 271 keV
4. G7 clover pulsers are beyond 5 MeV. No pulser for crystal G7Green
5. During the lasts dlt files (170613_1601_133Ba_009.dlt and 170613_1601_133Ba_010.dlt) the source was removed from the center of BRIKEN.
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325
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Tue Jun 13 07:35:35 2017 |
briken team | 133Ba calibration |
After experiment 133Ba calibration
Working directory: /data/1706FinalCalibrations
Configuration file: 170604_Conf_BrikenFull_AfterCrisis.xlsx
DLT file name: 170613_1533_133Ba_001.dlt
Start: 15:33
Stop: 15:59
Online rootfile: 133Ba_cal_z0_1533_1559_170613.root
COMMENTS:
1. Source centered in both BRIKEN and clovers (faced towards clover D4)
2. No AIDA in
3. D4 clover pulsers are at 253, 260, 265, and 271 keV
4. G7 clover pulsers are beyond 5 MeV. No pulser for crystal G7Green |
324
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Tue Jun 13 06:50:12 2017 |
Briken Colaboration | 152Eu calibration |
After experiment 152Eu calibration
Working directory: /data/1706FinalCalibrations
Configuration file: 170604_Conf_BrikenFull_AfterCrisis.xlsx
DLT file name: 170613_1451_152Eu_000.dlt
Start: 14:51
Stop: 15:24
Online rootfile:152Eu_cal_z0_1451_1524_170613.root
COMMENTS:
1. Source centered in both BRIKEN and clovers (faced towards clover D4)
2. No AIDA in
3. D4 clover pulsers are at 253, 260, 265, and 271 keV
4. G7 clover pulsers are beyond 5 MeV. No pulser for crystal G7Green |
Attachment 1: 170604_Conf_BrikenFull_AfterCrisis.xlsx
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323
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Tue Jun 13 05:18:07 2017 |
PV | How to install ELOG for BRIKEN campaign 2017a |
Get ELOG software including entries for BRIKEN campaign 2017a from mars computer:
briken@mars:/data01/2017data/briken/ur17a/elogBRIKEN2017a.tar.gz
To run and view the Elog website in your local computer
For Ubuntu 16
Please, update/install the following packages:
sudo apt-get install python-pip python-dev libffi-dev libssl-dev libxml2-dev libxslt1-dev libjpeg8-dev zlib1g-dev
- Extract the file:
tar -xvzf elogBRIKEN2017a.tar.gz
- Go to the extracted directory and execute make
cd elogBRIKEN2017a
make
- Run elogd service from that directory:
./elogd start
then it will display:
elogd 3.1.2 built Dec 8 2016, 13:24:26 revision bd75964
CKeditor detected
ImageMagick detected
Indexing logbooks ...
Create empty password file "logbooks/ribf.passwd"
done
Server listening on port 3333 ...
- Go to your web browser, enter
http://localhost:3333
- It will ask you to register a new elog account, fill in your preferred information
Login name: (name without space)
Full name:
Email:
Password:
Retype password:
and press Save button
- Next, it will ask you to choose which logbook you want to subscribe. Choose "BRIKEN2017-June" if you like, then press Save button at the top left corner
- The experimental log should be displayed then. Select BRIKEN > BRIKEN2017-June. |
322
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Mon Jun 12 22:28:02 2017 |
Oscar | The SUSHIRO app guide |
It's here...it's rough...but it hopefully gets the job done |
Attachment 1: SUSHIRO_For_Dummies_V001.pdf
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321
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Mon Jun 12 02:45:44 2017 |
Iris Dillmann AT | Setup detectors. Id of Ancillary@BRIKEN |
Attachment 1: Setup detectors
Attachment 2: example of configuration file (valid only for RIBF127). The Id of the ancillary detectors are:
DTPulser 95
V_PL_T 96
V_PL_B 97
F11_PL_R_LG 98
F11_PL_L_LG 99
V_NaI_R 100
V_NaI_L 101
F11_PL_R 102
F11_PL_L 103
Si_T 104
Si_B 105
AIDA_PL 106 |
Attachment 1: Setup-26May2017.png
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Attachment 2: OfflineConf_Signals.csv
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Name Id Crate ModId Type Index1 Index2 Channel Type Parameter Ethreshold(call) Emax(cal) EOffset EFactor TOffset TFactor Ebin Elow Ehigh Tbin Tlow Thigh NumOfCallSections Xlow Xhigh Offset Fact1 Fact2 Xlow Xhigh Offset Fact1 Fact2 Xlow Xhigh Offset Fact1 Fact2
He001 0 1 1 1 1 0 0 SIS3316 EFIR 120 10000 0 0.000807502 0 20 3500 0 3500 1000 0 200000 0
He002 1 1 1 1 1 0 1 SIS3316 EFIR 120 10000 0 0.0008051 0 20 3500 0 3500 1000 0 200000 0
He003 2 1 1 1 1 0 2 SIS3316 EFIR 120 10000 0 0.0008809222 0 20 3500 0 3500 1000 0 200000 0
He004 3 1 1 1 2 0 3 SIS3316 EFIR 120 10000 0 0.0008155797 0 20 3500 0 3500 1000 0 200000 0
He005 4 1 1 1 2 0 4 SIS3316 EFIR 120 10000 0 0.000797081 0 20 3500 0 3500 1000 0 200000 0
He006 5 1 1 1 3 0 5 SIS3316 EFIR 120 10000 0 0.001 0 20 3500 0 3500 1000 0 200000 0
He007 6 1 1 1 1 0 6 SIS3316 EFIR 120 10000 0 0.000791575 0 20 3500 0 3500 1000 0 200000 0
He008 7 1 1 1 1 0 7 SIS3316 EFIR 120 10000 0 0.000809329 0 20 3500 0 3500 1000 0 200000 0
He009 8 1 1 1 1 0 8 SIS3316 EFIR 120 10000 0 0.000809901 0 20 3500 0 3500 1000 0 200000 0
He010 9 1 1 1 2 0 9 SIS3316 EFIR 120 10000 0 0.000820137 0 20 3500 0 3500 1000 0 200000 0
He011 10 1 1 1 2 0 10 SIS3316 EFIR 120 10000 0 0.00078482 0 20 3500 0 3500 1000 0 200000 0
He012 11 1 1 1 3 0 11 SIS3316 EFIR 120 10000 0 0.000804308 0 20 3500 0 3500 1000 0 200000 0
He021 12 1 1 1 1 0 12 SIS3316 EFIR 120 10000 0 0.000883153 0 20 3500 0 3500 1000 0 200000 0
He022 13 1 1 1 2 0 13 SIS3316 EFIR 120 10000 0 0.000901874 0 20 3500 0 3500 1000 0 200000 0
He023 14 1 1 1 2 0 14 SIS3316 EFIR 120 10000 0 0.000881293 0 20 3500 0 3500 1000 0 200000 0
He024 15 1 1 1 3 0 15 SIS3316 EFIR 120 10000 0 0.000921597 0 20 3500 0 3500 1000 0 200000 0
He013 16 1 2 1 1 0 0 SIS3316 EFIR 120 10000 0 0.000883137 0 20 3500 0 3500 1000 0 200000 0
He014 17 1 2 1 1 0 1 SIS3316 EFIR 120 10000 0 0.000890012 0 20 3500 0 3500 1000 0 200000 0
He015 18 1 2 1 1 0 2 SIS3316 EFIR 120 10000 0 0.000892132 0 20 3500 0 3500 1000 0 200000 0
He016 19 1 2 1 2 0 3 SIS3316 EFIR 120 10000 0 0.000881072 0 20 3500 0 3500 1000 0 200000 0
He017 20 1 2 1 2 0 4 SIS3316 EFIR 120 10000 0 0.000884337 0 20 3500 0 3500 1000 0 200000 0
He018 21 1 2 1 3 0 5 SIS3316 EFIR 120 10000 0 0.000888505 0 20 3500 0 3500 1000 0 200000 0
He019 22 1 2 1 1 0 6 SIS3316 EFIR 120 10000 0 0.000892845 0 20 3500 0 3500 1000 0 200000 0
He020 23 1 2 1 1 0 7 SIS3316 EFIR 120 10000 0 0.000897665 0 20 3500 0 3500 1000 0 200000 0
He031 24 1 2 1 3 1 8 SIS3316 EFIR 120 10000 0 0.00126943 0 20 3500 0 3500 1000 0 200000 0
He032 25 1 2 1 3 1 9 SIS3316 EFIR 120 10000 0 0.00123783 0 20 3500 0 3500 1000 0 200000 0
He033 26 1 2 1 2 1 10 SIS3316 EFIR 120 10000 0 0.00127639 0 20 3500 0 3500 1000 0 200000 0
He034 27 1 2 1 2 1 11 SIS3316 EFIR 120 10000 0 0.00126828 0 20 3500 0 3500 1000 0 200000 0
He035 28 1 2 1 2 1 12 SIS3316 EFIR 120 10000 0 0.0012603 0 20 3500 0 3500 1000 0 200000 0
He036 29 1 2 1 2 1 13 SIS3316 EFIR 120 10000 0 0.00131271 0 20 3500 0 3500 1000 0 200000 0
He037 30 1 2 1 3 1 14 SIS3316 EFIR 120 10000 0 0.00131355 0 20 3500 0 3500 1000 0 200000 0
He038 31 1 2 1 3 1 15 SIS3316 EFIR 120 10000 0 0.00123794 0 20 3500 0 3500 1000 0 200000 0
He025 32 1 3 1 3 1 0 SIS3316 EFIR 120 10000 0 0.0012566 0 20 3500 0 3500 1000 0 200000 0
He026 33 1 3 1 1 1 1 SIS3316 EFIR 120 10000 0 0.00129234 0 20 3500 0 3500 1000 0 200000 0
He027 34 1 3 1 1 1 2 SIS3316 EFIR 120 10000 0 0.00131105 0 20 3500 0 3500 1000 0 200000 0
He028 35 1 3 1 1 1 3 SIS3316 EFIR 120 10000 0 0.00126285 0 20 3500 0 3500 1000 0 200000 0
He029 36 1 3 1 1 1 4 SIS3316 EFIR 120 10000 0 0.00128736 0 20 3500 0 3500 1000 0 200000 0
He030 37 1 3 1 1 1 5 SIS3316 EFIR 120 10000 0 0.00128879 0 20 3500 0 3500 1000 0 200000 0
He043 38 1 3 1 3 1 6 SIS3316 EFIR 120 10000 0 0.0014062 0 20 3500 0 3500 1000 0 200000 0
He044 39 1 3 1 3 1 7 SIS3316 EFIR 120 10000 0 0.00142331 0 20 3500 0 3500 1000 0 200000 0
He045 40 1 3 1 3 1 8 SIS3316 EFIR 120 10000 0 0.00138377 0 20 3500 0 3500 1000 0 200000 0
He046 41 1 3 1 1 1 9 SIS3316 EFIR 120 10000 0 0.00143469 0 20 3500 0 3500 1000 0 200000 0
He047 42 1 3 1 1 1 10 SIS3316 EFIR 120 10000 0 0.00141457 0 20 3500 0 3500 1000 0 200000 0
He048 43 1 3 1 1 1 11 SIS3316 EFIR 120 10000 0 0.00137187 0 20 3500 0 3500 1000 0 200000 0
He049 44 1 3 1 1 1 12 SIS3316 EFIR 120 10000 0 0.0014929 0 20 3500 0 3500 1000 0 200000 0
He050 45 1 3 1 1 1 13 SIS3316 EFIR 120 10000 0 0.00145672 0 20 3500 0 3500 1000 0 200000 0
He051 46 1 3 1 3 1 14 SIS3316 EFIR 120 10000 0 0.00143753 0 20 3500 0 3500 1000 0 200000 0
He052 47 1 3 1 3 1 15 SIS3316 EFIR 120 10000 0 0.00140445 0 20 3500 0 3500 1000 0 200000 0
He039 48 1 4 1 3 1 0 SIS3316 EFIR 120 10000 0 0.00144939 0 20 3500 0 3500 1000 0 200000 0
He040 49 1 4 1 3 1 1 SIS3316 EFIR 120 10000 0 0.00141155 0 20 3500 0 3500 1000 0 200000 0
He041 50 1 4 1 3 1 2 SIS3316 EFIR 120 10000 0 0.00140412 0 20 3500 0 3500 1000 0 200000 0
He042 51 1 4 1 3 1 3 SIS3316 EFIR 120 10000 0 0.00145083 0 20 3500 0 3500 1000 0 200000 0
He053 52 1 4 1 2 1 4 SIS3316 EFIR 120 10000 0 0.000539188 0 20 3500 0 3500 1000 0 200000 0
He054 53 1 4 1 2 1 5 SIS3316 EFIR 120 10000 0 0.000535295 0 20 3500 0 3500 1000 0 200000 0
He055 54 1 4 1 2 1 6 SIS3316 EFIR 120 10000 0 0.000550983 0 20 3500 0 3500 1000 0 200000 0
He056 55 1 4 1 2 1 7 SIS3316 EFIR 120 10000 0 0.00053126 0 20 3500 0 3500 1000 0 200000 0
He057 56 1 4 1 3 1 8 SIS3316 EFIR 120 10000 0 0.000544984 0 20 3500 0 3500 1000 0 200000 0
He058 57 1 4 1 3 1 9 SIS3316 EFIR 120 10000 0 0.000546973 0 20 3500 0 3500 1000 0 200000 0
He059 58 1 4 1 3 1 10 SIS3316 EFIR 120 10000 0 0.000540405 0 20 3500 0 3500 1000 0 200000 0
He060 59 1 4 1 3 1 11 SIS3316 EFIR 120 10000 0 0.000570587 0 20 3500 0 3500 1000 0 200000 0
He061 60 1 4 1 3 1 12 SIS3316 EFIR 120 10000 0 0.000542264 0 20 3500 0 3500 1000 0 200000 0
He062 61 1 4 1 3 1 13 SIS3316 EFIR 120 10000 0 0.000539482 0 20 3500 0 3500 1000 0 200000 0
He063 62 1 4 1 3 1 14 SIS3316 EFIR 120 10000 0 0.000546096 0 20 3500 0 3500 1000 0 200000 0
He064 63 1 4 1 3 1 15 SIS3316 EFIR 120 10000 0 0.000559717 0 20 3500 0 3500 1000 0 200000 0
He065 64 1 5 1 5 2 0 SIS3316 EFIR 120 10000 0 0.000640421 0 20 3500 0 3500 1000 0 200000 0
He066 65 1 5 1 4 2 1 SIS3316 EFIR 120 10000 0 0.000667932 0 20 3500 0 3500 1000 0 200000 0
He067 66 1 5 1 4 2 2 SIS3316 EFIR 120 10000 0 0.000651215 0 20 3500 0 3500 1000 0 200000 0
He068 67 1 5 1 5 2 3 SIS3316 EFIR 120 10000 0 0.000650567 0 20 3500 0 3500 1000 0 200000 0
He069 68 1 5 1 7 2 4 SIS3316 EFIR 120 10000 0 0.000654021 0 20 3500 0 3500 1000 0 200000 0
He070 69 1 5 1 7 2 5 SIS3316 EFIR 120 10000 0 0.000647755 0 20 3500 0 3500 1000 0 200000 0
He071 70 1 5 1 7 2 6 SIS3316 EFIR 120 10000 0 0.000669808 0 20 3500 0 3500 1000 0 200000 0
He072 71 1 5 1 7 2 7 SIS3316 EFIR 120 10000 0 0.000649558 0 20 3500 0 3500 1000 0 200000 0
He073 72 1 5 1 5 2 8 SIS3316 EFIR 120 10000 0 0.000661141 0 20 3500 0 3500 1000 0 200000 0
He074 73 1 5 1 4 2 9 SIS3316 EFIR 120 10000 0 0.000654012 0 20 3500 0 3500 1000 0 200000 0
He075 74 1 5 1 4 2 10 SIS3316 EFIR 120 10000 0 0.000671785 0 20 3500 0 3500 1000 0 200000 0
He076 75 1 5 1 5 2 11 SIS3316 EFIR 120 10000 0 0.000665415 0 20 3500 0 3500 1000 0 200000 0
He077 76 1 5 1 7 2 12 SIS3316 EFIR 120 10000 0 0.000654976 0 20 3500 0 3500 1000 0 200000 0
He078 77 1 5 1 7 2 13 SIS3316 EFIR 120 10000 0 0.000653886 0 20 3500 0 3500 1000 0 200000 0
He079 78 1 5 1 7 2 14 SIS3316 EFIR 120 10000 0 0.000655567 0 20 3500 0 3500 1000 0 200000 0
He080 79 1 5 1 7 2 15 SIS3316 EFIR 120 10000 0 0.000649916 0 20 3500 0 3500 1000 0 200000 0
He081 80 1 6 1 4 3 0 SIS3316 EFIR 120 10000 0 0.000557362 0 20 3500 0 3500 1000 0 200000 0
He082 81 1 6 1 4 3 1 SIS3316 EFIR 120 10000 0 0.000550055 0 20 3500 0 3500 1000 0 200000 0
He083 82 1 6 1 4 3 2 SIS3316 EFIR 120 10000 0 0.00050121 0 20 3500 0 3500 1000 0 200000 0
He084 83 1 6 1 4 3 3 SIS3316 EFIR 120 10000 0 0.000518147 0 20 3500 0 3500 1000 0 200000 0
He085 84 1 6 1 4 3 4 SIS3316 EFIR 120 10000 0 0.000539778 0 20 3500 0 3500 1000 0 200000 0
He086 85 1 6 1 5 3 5 SIS3316 EFIR 120 10000 0 0.000548182 0 20 3500 0 3500 1000 0 200000 0
He087 86 1 6 1 5 3 6 SIS3316 EFIR 120 10000 0 0.000545587 0 20 3500 0 3500 1000 0 200000 0
He088 87 1 6 1 5 3 7 SIS3316 EFIR 120 10000 0 0.000507506 0 20 3500 0 3500 1000 0 200000 0
He089 88 1 6 1 5 3 8 SIS3316 EFIR 120 10000 0 0.000511626 0 20 3500 0 3500 1000 0 200000 0
He090 89 1 6 1 5 3 9 SIS3316 EFIR 120 10000 0 0.00051489 0 20 3500 0 3500 1000 0 200000 0
He091 90 1 6 1 5 3 10 SIS3316 EFIR 120 10000 0 0.000505332 0 20 3500 0 3500 1000 0 200000 0
He092 91 1 6 1 6 3 11 SIS3316 EFIR 120 10000 0 0.000504664 0 20 3500 0 3500 1000 0 200000 0
He093 92 1 6 1 6 3 12 SIS3316 EFIR 120 10000 0 0.000512227 0 20 3500 0 3500 1000 0 200000 0
He094 93 1 6 1 6 3 13 SIS3316 EFIR 120 10000 0 0.000518939 0 20 3500 0 3500 1000 0 200000 0
He095 94 1 6 1 6 3 14 SIS3316 EFIR 120 10000 0 0.000516268 0 20 3500 0 3500 1000 0 200000 0
DTPulser 95 1 7 3 8 15 15 SIS3316 EFIR 120 10000 0 0.001 0 20 2000 0 3500 1000 0 200000 0
V_PL_T 96 1 7 3 9 1 0 SIS3316 EFIR 0 10000 0 0.018 0 20 2000 0 20000 1000 0 200000 0
V_PL_B 97 1 7 3 9 2 1 SIS3316 EFIR 0 10000 0 0.018 0 20 2000 0 20000 1000 0 200000 0
F11_PL_R_LG 98 1 7 3 10 1 4 SIS3316 EFIR 0 10000 0 0.00855 0 20 2000 0 20000 1000 0 200000 0
F11_PL_L_LG 99 1 7 3 10 2 5 SIS3316 EFIR 0 10000 0 0.00955 0 20 2000 0 20000 1000 0 200000 0
V_NaI_R 100 1 7 3 10 3 6 SIS3316 EFIR 0 10000 0 0.00127 0 20 2000 0 20000 1000 0 200000 0
V_NaI_L 101 1 7 3 10 4 7 SIS3316 EFIR 0 10000 0 0.000988 0 20 2000 0 20000 1000 0 200000 0
F11_PL_R 102 1 7 3 11 1 2 SIS3316 EFIR 0 10000 0 0.00855 0 20 2000 0 20000 1000 0 200000 0
F11_PL_L 103 1 7 3 11 2 3 SIS3316 EFIR 0 10000 0 0.00955 0 20 2000 0 20000 1000 0 200000 0
Si_T 104 1 7 3 12 1 12 SIS3316 EFIR 0 10000 0 0.000079702 0 20 2000 0 20000 1000 0 200000 0
Si_B 105 1 7 3 12 2 13 SIS3316 EFIR 0 10000 0 0.000079702 0 20 2000 0 20000 1000 0 200000 0
AIDA_PL 106 1 7 3 13 10 8 SIS3316 EFIR 0 10000 0 0.000247961 0 20 2000 0 20000 1000 0 200000 0
He096 107 2 1 1 6 3 0 SIS3302 EFIR 120 10000 0 0.000129852 0 20 3500 0 3500 1000 0 200000 0
He097 108 2 1 1 6 3 1 SIS3302 EFIR 120 10000 0 0.000131212 0 20 3500 0 3500 1000 0 200000 0
He098 109 2 1 1 6 3 2 SIS3302 EFIR 120 10000 0 0.000132759 0 20 3500 0 3500 1000 0 200000 0
He099 110 2 1 1 6 3 3 SIS3302 EFIR 120 10000 0 0.000131197 0 20 3500 0 3500 1000 0 200000 0
He100 111 2 1 1 6 3 4 SIS3302 EFIR 120 10000 0 0.000130307 0 20 3500 0 3500 1000 0 200000 0
He101 112 2 1 1 7 3 5 SIS3302 EFIR 120 10000 0 0.000131164 0 20 3500 0 3500 1000 0 200000 0
He102 113 2 1 1 7 3 6 SIS3302 EFIR 120 10000 0 0.000129263 0 20 3500 0 3500 1000 0 200000 0
He103 114 2 1 1 7 3 7 SIS3302 EFIR 120 10000 0 0.000131641 0 20 3500 0 3500 1000 0 200000 0
He104 115 2 2 1 7 3 0 SIS3302 EFIR 120 10000 0 0.000129631 0 20 3500 0 3500 1000 0 200000 0
He105 116 2 2 1 7 3 1 SIS3302 EFIR 120 10000 0 0.000131767 0 20 3500 0 3500 1000 0 200000 0
He106 117 2 2 1 7 3 2 SIS3302 EFIR 120 10000 0 0.000131115 0 20 3500 0 3500 1000 0 200000 0
He107 118 2 2 1 7 3 3 SIS3302 EFIR 120 10000 0 0.000144548 0 20 3500 0 3500 1000 0 200000 0
He108 119 2 2 1 7 3 4 SIS3302 EFIR 120 10000 0 0.000131547 0 20 3500 0 3500 1000 0 200000 0
He109 120 2 2 1 7 3 5 SIS3302 EFIR 120 10000 0 0.000132571 0 20 3500 0 3500 1000 0 200000 0
He110 121 2 2 1 7 3 6 SIS3302 EFIR 120 10000 0 0.000133191 0 20 3500 0 3500 1000 0 200000 0
He111 122 2 3 1 4 3 0 SIS3302 EFIR 120 10000 0 0.000127576 0 20 3500 0 3500 1000 0 200000 0
He112 123 2 3 1 4 3 1 SIS3302 EFIR 120 10000 0 0.000130547 0 20 3500 0 3500 1000 0 200000 0
He113 124 2 3 1 4 3 2 SIS3302 EFIR 120 10000 0 0.000128209 0 20 3500 0 3500 1000 0 200000 0
He114 125 2 3 1 4 3 3 SIS3302 EFIR 120 10000 0 0.00013208 0 20 3500 0 3500 1000 0 200000 0
He115 126 2 3 1 4 3 4 SIS3302 EFIR 120 10000 0 0.000132839 0 20 3500 0 3500 1000 0 200000 0
He116 127 2 3 1 5 3 5 SIS3302 EFIR 120 10000 0 0.000127298 0 20 3500 0 3500 1000 0 200000 0
He117 128 2 3 1 5 3 6 SIS3302 EFIR 120 10000 0 0.000129108 0 20 3500 0 3500 1000 0 200000 0
He118 129 2 3 1 5 3 7 SIS3302 EFIR 120 10000 0 0.000134917 0 20 3500 0 3500 1000 0 200000 0
He119 130 2 4 1 5 3 0 SIS3302 EFIR 120 10000 0 0.000134458 0 20 3500 0 3500 1000 0 200000 0
He120 131 2 4 1 5 3 1 SIS3302 EFIR 120 10000 0 0.000125501 0 20 3500 0 3500 1000 0 200000 0
He121 132 2 4 1 5 3 2 SIS3302 EFIR 120 10000 0 0.000128145 0 20 3500 0 3500 1000 0 200000 0
He122 133 2 4 1 6 3 3 SIS3302 EFIR 120 10000 0 0.000132339 0 20 3500 0 3500 1000 0 200000 0
He123 134 2 4 1 6 3 4 SIS3302 EFIR 120 10000 0 0.000132855 0 20 3500 0 3500 1000 0 200000 0
He124 135 2 4 1 6 3 5 SIS3302 EFIR 120 10000 0 0.000139105 0 20 3500 0 3500 1000 0 200000 0
He125 136 2 4 1 6 3 6 SIS3302 EFIR 120 10000 0 0.000130536 0 20 3500 0 3500 1000 0 200000 0
He126 137 2 5 1 6 3 0 SIS3302 EFIR 120 10000 0 0.000130205 0 20 3500 0 3500 1000 0 200000 0
He127 138 2 5 1 6 3 1 SIS3302 EFIR 120 10000 0 0.000130204 0 20 3500 0 3500 1000 0 200000 0
He128 139 2 5 1 6 3 2 SIS3302 EFIR 120 10000 0 0.000132938 0 20 3500 0 3500 1000 0 200000 0
He129 140 2 5 1 6 3 3 SIS3302 EFIR 120 10000 0 0.000133857 0 20 3500 0 3500 1000 0 200000 0
He130 141 2 5 1 6 3 4 SIS3302 EFIR 120 10000 0 0.000129359 0 20 3500 0 3500 1000 0 200000 0
He131 142 2 5 1 7 3 5 SIS3302 EFIR 120 10000 0 0.000134546 0 20 3500 0 3500 1000 0 200000 0
He132 143 2 5 1 7 3 6 SIS3302 EFIR 120 10000 0 0.000128561 0 20 3500 0 3500 1000 0 200000 0
He133 144 2 5 1 7 3 7 SIS3302 EFIR 120 10000 0 0.000137397 0 20 3500 0 3500 1000 0 200000 0
He134 145 2 6 1 7 3 0 SIS3302 EFIR 120 10000 0 0.000139181 0 20 3500 0 3500 1000 0 200000 0
He135 146 2 6 1 7 3 1 SIS3302 EFIR 120 10000 0 0.00013444 0 20 3500 0 3500 1000 0 200000 0
He136 147 2 6 1 7 3 2 SIS3302 EFIR 120 10000 0 0.000128301 0 20 3500 0 3500 1000 0 200000 0
He137 148 2 6 1 7 3 3 SIS3302 EFIR 120 10000 0 0.00012958 0 20 3500 0 3500 1000 0 200000 0
He138 149 2 6 1 7 3 4 SIS3302 EFIR 120 10000 0 0.000129081 0 20 3500 0 3500 1000 0 200000 0
He139 150 2 6 1 7 3 5 SIS3302 EFIR 120 10000 0 0.000132869 0 20 3500 0 3500 1000 0 200000 0
He140 151 2 6 1 7 3 6 SIS3302 EFIR 120 10000 0 0.000136463 0 20 3500 0 3500 1000 0 200000 0
D4Black 152 2 7 2 14 1 0 SIS3302 EFIR 15 10000 -0.6017825233 0.0015836325 0 20 16000 0 8000 1000 0 200000 0
D4Red 153 2 7 2 14 2 1 SIS3302 EFIR 15 10000 -0.2629124127 0.0015439776 0 20 16000 0 8000 1000 0 200000 0
D4Green 154 2 7 2 14 3 2 SIS3302 EFIR 15 10000 0.2931096096 0.0015329461 0 20 16000 0 8000 1000 0 200000 0
D4Blue 155 2 7 2 14 4 3 SIS3302 EFIR 15 10000 -0.0427639699 0.000664755 0 20 16000 0 8000 1000 0 200000 0
G7Black 156 2 7 2 15 1 4 SIS3302 EFIR 15 10000 -0.5577366054 0.00070 0 20 16000 0 8000 1000 0 200000 0
G7Red 157 2 7 2 15 2 5 SIS3302 EFIR 15 10000 -0.6254548603 0.000683305 0 20 16000 0 8000 1000 0 200000 0
G7Green 158 2 7 2 15 3 6 SIS3302 EFIR 15 10000 -0.1966707051 0.0006685615 0 20 16000 0 8000 1000 0 200000 0
G7Blue 159 2 7 2 15 4 7 SIS3302 EFIR 15 10000 -0.2212697416 0.0006968099 0 20 16000 0 8000 1000 0 200000 0
SyncPulser 160 1 6 3 8 15 15 SIS3316 EFIR 120 10000 0 0.001 0 20 2000 0 3500 1000 0 200000 0
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320
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Mon Jun 12 02:38:27 2017 |
JA AA AIM AT AT | VME crate & new configuration |
Sun Jun 4 2017 11:16:45 VME crate #1 crashed
New configuration file of BRIKEN
Main changes:
-VME address of digitizer V1A1 (now address #7, instead of #1)
-Digitizer for Ancillary now placed at VME crate #2, VME address #8
In the offline configuration file only these addresses can be changed, keeping the same Id |
Attachment 1: 170603_Conf_BrikenFull.xlsx
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Draft
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Mon May 29 07:06:56 2017 |
K. Matsui | Energy loss in Long Plastic Scintillator |
After Al degrader with the optimized width of 13 mm, the energy loss in Long Plastic Scintillator is 546(2) MeV at F11.
This value depends on |
Draft
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Mon May 29 05:40:49 2017 |
K. Matsui | energy loss at logn |
|
317
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Mon May 29 04:17:34 2017 |
YS | Clover Efficiency |
Clover gamma detection efficiency calculation with 152Eu
Date of the measurement: 2017-05-26 10:15
root file: 170526_1015_152Eu_noAIDA_z0cm_014.root
Gamma Energy[keV] {121.781700, 244.697500, 344.278500, 444.000000, 778.904500, 867.378000, 964.100000,
1112.074000, 1408.011000}
Crystal ID 152 Efficiency[%] {1.536508, 0.978779, 0.736707, 0.591553, 0.359426, 0.338228, 0.300229, 0.272331,
0.220314}
Crystal ID 152 Efficiency Error {0.030465, 0.021204, 0.014732, 0.016358, 0.008284, 0.011340, 0.006673,
0.006173, 0.004757}
Crystal ID 153 Efficiency[%] {1.679147, 1.051609, 0.799702, 0.628184, 0.386672, 0.387489, 0.328493, 0.300337,
0.236573}
Crystal ID 153 Efficiency Error {0.033341, 0.023338, 0.016004, 0.017827, 0.008906, 0.013626, 0.007298,
0.006773, 0.005071}
Crystal ID 154 Efficiency[%] {1.402847, 0.922081, 0.696455, 0.593818, 0.348820, 0.341118, 0.298197, 0.276055,
0.215494}
Crystal ID 154 Efficiency Error {0.027933, 0.020478, 0.014004, 0.017865, 0.008087, 0.012283, 0.006708,
0.006288, 0.004660}
Crystal ID 155 Efficiency[%] {1.329735, 0.886053, 0.665180, 0.559708, 0.340513, 0.340755, 0.288800, 0.261229,
0.202480}
Crystal ID 155 Efficiency Error {0.026511, 0.020274, 0.013378, 0.016628, 0.007732, 0.010686, 0.006432,
0.005958, 0.004413}
Crystal ID 156 Efficiency[%] {1.163705, 0.757446, 0.548990, 0.465020, 0.282777, 0.294110, 0.237165, 0.220572,
0.155430}
Crystal ID 156 Efficiency Error {0.023277, 0.017832, 0.011114, 0.014924, 0.006765, 0.010733, 0.005496,
0.005160, 0.003514}
Crystal ID 157 Efficiency[%] {1.420320, 0.906654, 0.672645, 0.536032, 0.347827, 0.346548, 0.298879, 0.269536,
0.196238}
Crystal ID 157 Efficiency Error {0.028367, 0.020536, 0.013537, 0.016528, 0.008115, 0.012147, 0.006664,
0.006128, 0.004314}
Crystal ID 158 Efficiency[%] {1.271836, 0.790926, 0.591132, 0.494340, 0.311442, 0.295866, 0.255764, 0.227822,
0.168103}
Crystal ID 158 Efficiency Error {0.025589, 0.018723, 0.011955, 0.015706, 0.007457, 0.010690, 0.005849,
0.005296, 0.003762}
Crystal ID 159 Efficiency[%] {1.268501, 0.806356, 0.588627, 0.511611, 0.297958, 0.326487, 0.252316, 0.231872,
0.175679}
Crystal ID 159 Efficiency Error {0.025339, 0.018906, 0.011939, 0.016912, 0.007159, 0.011892, 0.005740,
0.005411, 0.003900}
Total Efficiency[%] {11.072600, 7.099903, 5.299439, 4.380266, 2.675436, 2.670601, 2.259844, 2.059754, 1.570310}
Total Efficiency Error {0.078525, 0.057205, 0.037954, 0.047007, 0.022172, 0.033133, 0.018054, 0.016749, 0.012242}
Fitting Function: 10^{p_0 + p_1*ln(x) + p_2*ln^2(x) + p_3/x^2} (This is the function used in the textbook
"Radiation detection and measurement" by G.Knoll)
Parameters
Total (two clovers):
p_0 = 2.29172e-01 +/- 1.13185e-02
p_1 = 9.48436e-01 +/- 8.89344e-04
p_2 = -1.54934e-01 +/- 7.58240e-05
p_3 = 1.89920e+06 +/- 1.18292e+09
ID152:
FCN=1.11317 FROM HESSE STATUS=NOT POSDEF 23 CALLS 325 TOTAL
EDM=1.40411e-09 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 8.09248e+00 4.00474e-02 1.92940e-06 7.13568e-03
2 p1 -2.02411e+00 8.19548e-03 4.82585e-07 4.27674e-02
3 p2 9.78402e-02 1.18086e-03 2.33269e-08 2.59077e-01
4 p3 -2.11550e+09 1.97563e+08 5.04375e+02 2.35344e-13
ID153:
FCN=7.1582 FROM HESSE STATUS=NOT POSDEF 23 CALLS 345 TOTAL
EDM=1.28369e-11 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 5.98204e+00 4.02864e-02 1.42623e-06 1.27251e-03
2 p1 -1.30120e+00 8.24403e-03 3.10231e-07 7.00775e-03
3 p2 3.70097e-02 1.18706e-03 2.80719e-08 3.85335e-02
4 p3 -1.43256e+09 1.97976e+08 3.41550e+02 1.75334e-14
ID154:
FCN=7.31777 FROM HESSE STATUS=NOT POSDEF 23 CALLS 300 TOTAL
EDM=7.25203e-09 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 4.60707e+00 4.07462e-02 1.09841e-06 -1.28042e-02
2 p1 -8.62719e-01 8.33215e-03 2.05688e-07 -8.63564e-02
3 p2 9.84262e-04 1.20127e-03 2.86738e-08 -5.66097e-01
4 p3 -1.45278e+09 2.00179e+08 3.46370e+02 5.24463e-13
ID155:
FCN=8.93044 FROM HESSE STATUS=NOT POSDEF 23 CALLS 325 TOTAL
EDM=1.56376e-09 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 3.36149e-01 4.05951e-02 1.02424e-06 1.66747e-02
2 p1 5.96907e-01 8.27701e-03 1.78992e-07 9.42383e-02
3 p2 -1.24128e-01 1.19514e-03 3.10496e-08 5.35879e-01
4 p3 -5.49707e+08 1.98933e+08 1.31060e+02 2.34852e-13
ID156:
FCN=27.107 FROM HESSE STATUS=NOT POSDEF 23 CALLS 369 TOTAL
EDM=1.72237e-10 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 -6.26350e+00 4.21430e-02 1.78695e-06 -4.63010e-03
2 p1 2.85365e+00 8.58127e-03 6.80363e-07 -2.64484e-02
3 p2 -3.19389e-01 1.24245e-03 7.61484e-08 -1.51241e-01
4 p3 1.16616e+09 2.05264e+08 2.78034e+02 -1.93778e-14
ID157:
FCN=19.4716 FROM HESSE STATUS=NOT POSDEF 23 CALLS 342 TOTAL
EDM=1.04278e-08 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 -3.89605e+00 4.09683e-02 1.48832e-06 3.26076e-02
2 p1 2.04214e+00 8.37584e-03 4.86884e-07 1.83059e-01
3 p2 -2.47352e-01 1.20710e-03 5.89732e-08 1.02761e+00
4 p3 9.13701e+08 2.00155e+08 2.17843e+02 1.24035e-13
ID158:
FCN=7.59955 FROM HESSE STATUS=NOT POSDEF 23 CALLS 331 TOTAL
EDM=1.78742e-08 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 -8.46924e+00 4.17987e-02 2.01922e-06 -1.01596e-03
2 p1 3.60905e+00 8.55091e-03 8.60466e-07 8.06431e-03
3 p2 -3.83202e-01 1.23257e-03 9.13624e-08 1.28451e-01
4 p3 1.94705e+09 2.02809e+08 4.64212e+02 1.90916e-13
ID159:
FCN=24.8135 FROM HESSE STATUS=NOT POSDEF 27 CALLS 314 TOTAL
EDM=7.91895e-10 STRATEGY= 1 ERR MATRIX NOT POS-DEF
EXT PARAMETER APPROXIMATE STEP FIRST
NO. NAME VALUE ERROR SIZE DERIVATIVE
1 p0 -1.15142e+00 4.18270e-02 1.70735e-06 3.54687e-03
2 p1 1.09795e+00 8.55588e-03 2.98767e-07 1.75400e-02
3 p2 -1.67863e-01 1.23250e-03 5.18807e-08 8.63094e-02
4 p3 1.96354e+08 2.02197e+08 4.87057e+05 3.05910e-13
For comparison: EURICA total efficiency - see attachment 3 |
Attachment 1: eff_crystal.pdf
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Attachment 2: eff_total.pdf
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Attachment 3: EURICA_efficiency.jpg
|
|
316
|
Sun May 28 11:41:24 2017 |
YS | CLOVER energy calibration |
Clover calibration with 152Eu
Used peaks [keV]: 121.7817, 244.6975, 344.2785, 444.000, 778.9045, 867.378, 964.100, 1112.074, 1408.011
Up to 444keV is lower energy region, above 778.9045 is higher energy region.
All the peaks were fitted with Gaussian + Second Order Plolinomial(background) + Step Function(background).
Parameters: Second Order, First Order, Offset
ID 152 Lower: 1.14254e-08, 1.57915, 408.94
ID 152 Higher: -3.90753e-10, 1.58167, 1224.11
ID 153 Lower: -7.33088e-09, 1.54588, 264.002
ID 153 Higher: 4.72241e-09, 1.53548, 3541.56
ID 154 Lower: -4.45069e-08, 1.54978, -626.916
ID 154 Higher: -4.48059e-08, 1.58933, -14795.7
ID 155 Lower: -5.93726e-10, 0.666536, 230.739
ID 155 Higher: 1.74281e-09, 0.659392, 3973.56
ID 156 Lower: -4.00636e-09, 0.708287, -509.227
ID 156 Higher: 9.5416e-11, 0.705004, -1574.59
ID 157 Lower: -2.94588e-09, 0.686728, -572.626
ID 157 Higher: 3.24943e-10, 0.683273, -1684.07
ID 158 Lower: 1.30198e-09, 0.668335, 485.045
ID 158 Higher: -4.572e-10, 0.67108, -3189.18
ID 159 Lower: -4.37028e-09, 0.701927, -666.22
ID 159 Higher: 3.40354e-09, 0.685865, 8115.55 |
315
|
Sat May 27 11:19:57 2017 |
AIM, AT | AIDA+BRIKEN background |
Background measurement AIDA+BRIKEN
AIDA is inside BRIKEN
AIDA was taking data.
Start: run 31 subrun 41
Stop: run 41 subrun 239
BRIKEN started later.
Start: 27th-May, 19:19
Stop: 28th-May, around 11:00
DLT File name:170527_1919_bck_AIDAinside_022.dlt
RUN numbers: 022-024
RootFile: 170527_1919_1914_bck_AIDAin.root
Comments: at 28th-May, 19:17, reset time stamp |
314
|
Sat May 27 10:36:20 2017 |
JA,AT,JLT | BRIKEN DACQ |
Manuals for BRIKEN DACQ:
GasificShort.pdf including "Run protocol"
and Gasific70Manual.pdf (long) |
Attachment 1: Gasific70Manual.pdf
|
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Attachment 2: GasificShort.pdf
|
|
312
|
Sat May 27 04:46:55 2017 |
AIM | sources info |
Here is the sunflower webpage with information on the calibration sources:
http://www.nishina.riken.jp/collaboration/SUNFLOWER/misc/util/ribfsource.html |
311
|
Fri May 26 14:42:12 2017 |
JL, AT | Background |
Background measurement (no AIDA)
Configuration file: 170526_Conf_BrikenFull.xlsx
Start: 26th-May, at 22:51
Stop: 27th-May, at 09:54
DLT: 170526_2251_bck_noAIDA_019.dlt
RUN: 019-020
RootFile:170526_2251_0954_bck_noAIDA.root
Comments: run 018 was dummy (time reset needed) |
310
|
Fri May 26 14:27:08 2017 |
AIM, AT | BRIKEN Configuration File |
New configuration file of BRIKEN
Changes of 26th-May-2017
Previous config file 24th-May-2017
After the 152Eu calibration, the threshold of
>> V2A7C4 was increased from 20 to 30.
>> V2A7C6 was increased from 30 to 40.
AIDA veto plastic (40cm after the stack of DSSD) and
the silicon detector (shielding hole) were calibrated
with the Compton edge of 137Cs (891keV). |
Attachment 1: 170526_Conf_BrikenFull.xlsx
|
308
|
Fri May 26 09:07:46 2017 |
J. Agramunt | Synchronization Monitoring |
We started the synchronization monitoring programs to check that
it is OK as can be seen in the figure below
We are using the same scheme used during Ahn parasitic run,
namely the synchronization check signal is the BigRIPS trigger
signal send by them to us (AIDA, BRIKEN).
The monitorization procedure is different from the one used
in 2016. The description to lauch the processes is described
here below and in the attached PDF.
***********
To Launch the processes:
Open 4 terminals:
Terminal 1 (DataSink) type:
>ssh aida@d05
>cd /home/aida/DataPackage/DataSink/Linux64
>DataSink -i 3
Terminal 2 (SynCheck) type:
>ssh aida@d05
>cd /home/aida/SyncCheck
>./SynCheck
Terminal 3 (BigRIPS Data Relay) type:
>ssh aida@d05
>cd /home/aida/ribfts/ribftssender
>./ribftssender_mar17ca debug
(specific for current 40Ca parasitic run because we are not sending
a pulse signal to BigRIPS as trigger but receiving triggers from
BigRIPS to create the pulses)
Terminal 4 (AIDA Data Relay) type:
>npg@aidas1
>DataRelayFilter -n 10.32.0.12 -p 10307 -I 2
"-I 2" selects ID 2 as the one for the AIDA data stream,
which must correspond to the one expected by the DataSink in the d05 PC.
The programming transmitting the data from AIDA to the DataSink includes an
intermediate filtering step. This selects only correlation scalers from one
module (and possibly ADC values from one channel in that module).
Gasific MainWindow (Briken Data Relay):
In the DAQ Control tab: Click "Start Sync Monitoring" button.
In the pop up window set server ip and port (ip:10.32.0.12, port:10305)
By default this perform a check on the differences RIBF-BRIKEN and AIDA-BRIKEN.
In case that BRIKEN is not running, the option "SynCheck -M 1" check the differences
AIDA-RIBF and BRIKEN-RIBF, while "SynCheck -M 2" checks RIBF-AIDA and BRIKEN-AIDA
To synchronize:
In the Gasific MainWindow, DAQ Control tab: Click "Send Sync Pulse" button |
Attachment 1: synchroCheck.png
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Attachment 2: SynchronizationMonitoring.pdf
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307
|
Fri May 26 04:20:54 2017 |
JLT,AA,AT | CLOVER 60Co |
60Co No AIDA, Efficiency calibration
Start: 12:21
Stop: 12:50
Files:
170526_1221_60Co_noAIDA_z0cm_017.dlt
170526_1221_1250_60Co_z0cm.root |
306
|
Fri May 26 03:52:23 2017 |
AT,AA,JLT | CLOVER, 137Cs |
137Cs, No AIDA, Efficiency calibration
Source ID: 393
Same type as 133Ba
Start: 11:51
Stop: 12:10
Files:
170526_1151_137Cs_noAIDA_z0cm_016.dlt
170526_1151_1210_137Cs_z0cm.root |
305
|
Fri May 26 03:24:38 2017 |
GK,VP, AT, AA | CLOVER, 133Ba |
133Ba source efficiency calibration, no AIDA
Start: 11:23
Stop: 11:43
Files:
170526_1123_133Ba_noAIDA_z0cm_015.dlt
170526_1123_1143_133Ba_z0cm.root |
304
|
Fri May 26 02:17:40 2017 |
AT, AIM, JLT,AA, PV, KM | 152Eu |
Calibration with 152Eu source.
START time:10:15
DLT:170526_1015_152Eu_noAIDA_z0cm_014.dlt
STOP time:11:16
ROOT:170526_1015_1116_152Eu_z0cm.root
COMMENTS:
1. Source centered in both BRIKEN and clovers
2. No AIDA in
3. D4 clover pulsers are at 253, 260, 265, and 271 keV
4. G7 clover pulsers are beyond 5 MeV. No pulser for crystal G7Green |
303
|
Thu May 25 14:31:46 2017 |
AT, JLT, AA, AIM | Background measurement |
Background, No AIDA
Start:22:31
Stop: 09:24
dlt files: 170525_2231_bck_noAIDA_z0cm_010.dlt
run: 010-011-012
root file: 170525_2231_0924_bck_noAIDA_z0cm.root |
Attachment 1: 170525_ring1_bckg_run.png
|
|
Attachment 2: 170525_ring2_bckg_run.png
|
|
Attachment 3: 170525_ring3_bckg_run.png
|
|
Attachment 4: 170525_ring4_bckg_run.png
|
|
Attachment 5: 170525_ring5_bckg_run.png
|
|
Attachment 6: 170525_ring6_bckg_run.png
|
|
Attachment 7: 170525_ring7_bckg_run.png
|
|
302
|
Thu May 25 13:56:00 2017 |
AT, JLT, AA | 252Cf |
252Cf source in Z=0cm position.
Start:21:57
Stop: 22:26
Files
170525_2157_252Cf_z0cm_008.dlt
170525_2157_2226_252Cf_z0cm.root
The time stamp was reset finally (at the third try !!!)
There is a file 170525_2154_252Cf_z0cm_007.dlt which was taken for a short time, until we noticed again that the
time stamp was not reset. |
301
|
Thu May 25 13:42:45 2017 |
AT, PC,KR,JLT,AA | 252Cf |
252Cf source in Z=0cm position.
Start:21:41
Stop:21:52
Files
170525_2141_252Cf_z0cm_006.dlt
170525_2141_2152_252Cf_z0cm.root
We realized that the time stamp was not reset. |
300
|
Thu May 25 13:38:11 2017 |
AT, PC, KR, JLT, AA | Clover, detectors in new position |
Both clover detectors were moved. They are in a symmetrical position. The end on the clover nose is of the order
of 3-4 mm from the AIDA tunnel.
See sketch of CLOVERS with respect to beam.
See photos of the insertion distance of
both CLOVERS |
Attachment 1: CLOVER-sketch.jpg
|
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Attachment 2: D4-insertion.jpg
|
|
Attachment 3: G7-insertion.jpg
|
|
299
|
Thu May 25 13:24:02 2017 |
AT,PC,KR,JLT,AA | CLOVER, detector not in its rigth position |
We have noticed that D4 is not in its right position. That explains the different number of counts in the
detectors.
Probably of the order of 3 cm away from its nominal place.
The position of the other detector should be also checked.
Efficiency calibrations need to be repeated |
298
|
Thu May 25 12:53:47 2017 |
AT, PC, JLT, KR, AA | Clover, 60Co |
60Co source
Source ID: CD395
same type as 133Ba source
Start: 20:57
Stop:21:18
Position: z=0 cm, No AIDA
Pulser connected
There was an small file (dlt) before this run with no pulser connected (170525_2054_60Co_z0cm_004.dlt),
that run for only 3-4 min.
Files
170525_2057_60Co_z0cm_005.dlt
170525_2057_2118_60Co_z0cm_pulser.root
Comment: we noticed that the two clovers had different statistics for the 1332 peak. To be checked why
(source not in place ?)
The pulser shows similar counts, so the reason can not be deadtime
Answer: the D4 was not in its right position !!!!, efficiency calibrations have to be repeated :-( |
297
|
Thu May 25 12:49:55 2017 |
AT, JLT,PC,AA | Clover, 133Ba, LN2 filling |
We started the measurement of the source when the N2 filling started. Just to check if there are funny things
related to the filling.
Start: 18:45
Stop: 20:48
The source was in position z=0 cmm (no AIDA)
File name: 170525_1845_2048_133Ba_NFilling_z0cm_noD4Pulser.root |
296
|
Thu May 25 10:15:02 2017 |
A.T, G. K, A.M, A. A | CLOVER, 133Ba no pulser |
Source in position z=0 with the carton (cardboard) high-end, high-tech holder, but no AIDA (of course).
No pulser. Remember that the pulser is providing peaks around
Start: 18:11
Stop: 18:31
Files
170525_1811_133Ba_z0cm_003.dlt
170525_1831_133Ba_z0cm_noD4Pulser.root |
295
|
Thu May 25 09:51:37 2017 |
A.T, A.A | CLOVER, Ba133 |
Source details:
Diameter: 25.05 mm
Dz: 3 mm
Source ID: CD 392
With pulser
Start:17:45
Stop: 18:08
Files saved:
170525_1146_152Eu_z0cm_D4Pulser.root
170525_1745_133Ba_z0cm_PulserD4_002.dlt
Ps. See that the pulser generates peaks in the region 250-270 keV (to avoid people to invent new levels (and
gammas) populated
in the beta decay of 133Ba). |
Attachment 1: 170525_133Ba_D4_D4pulser.png
|
|
294
|
Wed May 24 13:22:46 2017 |
JLT,AT,KR,SG,RY,... | CLOVER 152Eu |
We connect the pulser to both CLOVERs
G7: It looks OK except for the G7-Green as before
(there pulser peak in the spectrum)
D4: the pulser peak appears at very low energies (200-600keV)
there seems to be a problem with pulser processing in the preamplifiers.
Should we still use it? We remove for the moment.
152Eu source calibration.
We put the 152Eu source at the center (on the cardboard)
and check de energy calibration. For most of the crystals
the calibration from March was pretty good except for D4-Red
that the gain changed by a factor 1/2 and D4-blue that changed by 2 (!?)
We redo the calibration:
G7: the resolution at 1.4MeV is 2.7keV
D4: the resolution at 1.4MeV is 3.9keV
DLT File; 170525_0947_152Eu_z0cm.root_000.dlt
RUN Number; 000
RootFile: 170525_1034_152Eu.root
Comments: rate of the clovers increased from 2000cps to 2400cps
for 10 min (from TS = 41.8E6 ms to TS = 42.4E6 ms)
We plugged the pulser in clover D4.
DLT File: 170525_0947_152Eu_z0cm_PulserD4_001.dlt
RUN Number: 001
RootFile: 170525_1146_152Eu_z0cm_D4Pulser.root
Source dimensions:
Diameter: 24.98 mm
DZ= 5.98 mm
Source ID: Ref 272, 09/9011
Source label up |
Attachment 1: 170525_152Eu_CloversRate.png
|
|
293
|
Wed May 24 06:42:05 2017 |
JLT,AT,AM,RY,SG | START Preparation |
We start to check every thing for the coming run
New directory: /data/1705Preparation/
Copy last configuration file of Ahn parasitic run
renamed:170524_Conf_BrikenFull.xlsx
252Cf source at the center.
Root file: 170524_252Cf_1st.root
Issues:
Pulsers of He006, He140 are tripled
There is a strange background above n-peak in He034
Calibration is ok except for He003, He004 and He006 !!!!
|
292
|
Sun Apr 2 16:18:57 2017 |
All | END OF PARASITIC RUN |
|
291
|
Sun Apr 2 01:04:24 2017 |
JLT ID JA GK CG VP YS Liu | Background |
Date: 2/04/2017
Start: 09:05
BRIKEN run: 76
DLT:170402_0905_Background_076.dlt
BRIKEN Rate: 1 cps
F11 Rate: 12 cps
Date: 3/04/2017
Stop:00:15
BRIKEN run: 78
Root file:170403_0905_0015_B076_B078_Background.root
OBSERVATIONS: AIDA was moved out at about 13:00 |
290
|
Sun Apr 2 00:44:01 2017 |
ID JA GK CG VP Liu JLT | 39Al run 75 |
Date: 2/04/2017
Start: 08:42
BRIKEN run: 75
AIDA Run: R24_0
BigRIPS run: 254
DLT:170402_0842_39Al_075.dlt
BRIKEN Rate: 1 cps
F11 Rate: 12 cps
Date: 2/04/2017
Stop:09:00
BRIKEN run: 75
AIDA Run: r24_4
BigRIPS run: 254
Root file:170402_0842_0900_B075_Al39.root
OBSERVATIONS: |
289
|
Sun Apr 2 00:19:01 2017 |
ID JA GK CG YS SN Liu VP | 39Al run 74 |
Date: 2/04/2017
Start: 08:17
BRIKEN run: 74
AIDA Run: R21_23
BigRIPS run: 252
DLT:170402_0817_39Al_074.dlt
BRIKEN Rate: 48 cps
F11 Rate: 320 cps
Date: 2/04/2017
Stop:08:20
BRIKEN run: 74
AIDA Run: r21_23
BigRIPS run: 252
Root file:170402_0817_0820_B074_Al39.root
OBSERVATIONS: |
288
|
Sat Apr 1 22:41:22 2017 |
ID, GK, SN, Liu YS JLT | 38Mg run 73 |
Date: 2/04/2017
Start: 06:37
BRIKEN run: 73
AIDA Run: R21_0
BigRIPS run: 237
DLT:170402_0637_38Mg_073.dlt
BRIKEN Rate: 5 -> 90 cps
F11 Rate: 30 -> 350 cps
Date: 2/04/2017
Stop: 08:06
BRIKEN run: 73
AIDA Run: r21_22
BigRIPS run: 251
Root file:170402_0637_0806_B073_Mg38.root
OBSERVATIONS:
Playing with degraders
Final degrader: 23mm
New BigRIPS run 238 started at 6:46 (38Mg beam attenuated by 1/8) -> very few counts in Si
New run 239-240 started at 7:03 (38Mg beam attenuated 1/2 narrow slit)-> we see more counts in the Si
run 241-242 atarted at 7:09 (38Mg 70% narrow slit)
run 243-244 at 7:16 (38Mg 5000enA)
run 245-246 at 7:23 (38Mg beam intensity 0.8)
run 247-248 at 7:32 (38Mg beam intensity 0.9)
run 249-250 at 7:38 (38Mg full beam)
run 251 at 7:41 (38Mg yield measurement) |
287
|
Sat Apr 1 22:18:00 2017 |
Liu, YS, CG, GK, SN, JLT | 38Mg run 72 |
DUMMY |
286
|
Sat Apr 1 21:37:42 2017 |
YS, Liu, CG | 37Na run 71 |
Date: 2/04/2017
Start:04:47
BRIKEN run: 71
AIDA Run: R20_410
BigRIPS run: 227
DLT:170402_0447_Na37_071.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 05:29
BRIKEN run: 71
AIDA Run: R20_420
BigRIPS run: 227
Root file:
OBSERVATIONS: The beam with this setting is finished and the BigRIPS team starts calibration runs. The beam will
not be delivered to ZDS. |
285
|
Sat Apr 1 19:48:41 2017 |
YS,CG,LIU | 37Na,run 70 |
Date: 2/04/2017
Start:03:47
BRIKEN run: 70
AIDA Run: R20_394
BigRIPS run: 226
DLT:170402_0347_Na37_070.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 04:47
BRIKEN run: 70
AIDA Run: R20_410
BigRIPS run: 226 |
284
|
Sat Apr 1 18:48:20 2017 |
YS, LIU, CG | 37Na run 69 |
Date: 2/04/2017
Start:02:47
BRIKEN run: 69
AIDA Run: R20_381
BigRIPS run: 225
DLT:170402_0247_Na37_069.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 03:46
BRIKEN run: 69
AIDA Run: R20_394
BigRIPS run: 225
Root file:
OBSERVATIONS: |
283
|
Sat Apr 1 17:45:01 2017 |
YS,CG,LIU | 37Na, run 68 |
Date: 2/04/2017
Start:01:44
BRIKEN run: 68
AIDA Run: R20_365
BigRIPS run: 224
DLT:170402_0144_Na37_068.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 02:46
BRIKEN run: 68
AIDA Run: R20_381
BigRIPS run: 224
Root file:
OBSERVATIONS: |
282
|
Sat Apr 1 16:17:59 2017 |
YS,CG, LIU | 37Na run 67 |
Date: 2/04/2017
Start:00:17
BRIKEN run: 67
AIDA Run: R20_345
BigRIPS run: 223
DLT:170402_0017_Na37_067.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 01:41
BRIKEN run: 67
AIDA Run: R20_364
BigRIPS run: 223
Root file:
OBSERVATIONS: beam was stopped at 01:41 |
281
|
Sat Apr 1 15:16:45 2017 |
JLT OH VP Liu YS | 37Na run 66 |
Date: 1/04/2017
Start:23:13
BRIKEN run: 66
AIDA Run: R20_330
BigRIPS run: 222
DLT:170401_2313_Na37_066.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 2/04/2017
Stop: 00:16
BRIKEN run: 66
AIDA Run: R20_345
BigRIPS run: 222
Root file:
OBSERVATIONS: |
280
|
Sat Apr 1 14:21:31 2017 |
PV OH Liu JLT | 37Na run 65 |
Date: 1/04/2017
Start:22:12
BRIKEN run: 65
AIDA Run: R20_317
BigRIPS run: 221
DLT:170401_2220_Na37_065.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 23:13
BRIKEN run: 65
AIDA Run: R20_330
BigRIPS run: 221
Root file:170401_2212_2312_B065_Na37.root
OBSERVATIONS: online cleared |
279
|
Sat Apr 1 13:15:37 2017 |
JA ID OH PV | Na37 Ne36 Run 064 |
Date: 1/04/2017
Start:21:13
BRIKEN run: 63
AIDA Run: R20_302
BigRIPS run: 220
DLT:170401_2015_Na37_063.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 22:12
BRIKEN run: 63
AIDA Run: R20_315
BigRIPS run: 220
Root file: 170401_2113_2212_B064_Na37.root
OBSERVATIONS: |
278
|
Sat Apr 1 12:15:21 2017 |
PV, OH, JLT, ID, JA | 37Na run 63 |
Date: 1/04/2017
Start:20:15
BRIKEN run: 63
AIDA Run: R20_287
BigRIPS run: 219
DLT:170401_2015_Na37_063.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 21:13
BRIKEN run: 63
AIDA Run: R20_302
BigRIPS run: 219
Root file: 170401_1909_2113_B063_Na37.root
OBSERVATIONS: |
277
|
Sat Apr 1 11:13:42 2017 |
PV,OH,JLT | 37Na run 62 |
Date: 1/04/2017
Start:19:09
BRIKEN run: 62
AIDA Run: R20_272
BigRIPS run: 218
DLT:170401_1913_Na37_062.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 20:13
BRIKEN run: 62
AIDA Run: R20_287
BigRIPS run: 218
Root file: 170401_1909_2013_B062_Na37.root
OBSERVATIONS: Degrader thickness was reduced by 1mm |
276
|
Sat Apr 1 10:26:07 2017 |
VP,OH,JLT | 37Na run 61 |
Date: 1/04/2017
Start:18:25
BRIKEN run: 61
AIDA Run: R20_259
BigRIPS run: 216
DLT:170401_1825_Na37_061.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 19:09
BRIKEN run: 61
AIDA Run: R20_271
BigRIPS run: 216
Root file:
OBSERVATIONS: We restarted the DACQ (and the synchronization)
because the program was refusing to save the ROOT file with histograms
New Conf file:170401_Conf_BrikenFull.xlsx
(contains the changes made online before (see entry 273) |
275
|
Sat Apr 1 10:15:44 2017 |
VP,OH,JLT | 37Na run 60 |
Date: 1/04/2017
Start:17:40
BRIKEN run: 60
AIDA Run: R20_247
BigRIPS run: 215
DLT:170401_1740_Na37_060.dlt
BRIKEN Rate: 1.6 cps
F11 Rate: 8. cps
Date: 1/04/2017
Stop: 18:05
BRIKEN run: 60
AIDA Run: R20_254
BigRIPS run: 215
Root file:
OBSERVATIONS:stop because of schange of stripper foil |
274
|
Sat Apr 1 08:39:47 2017 |
ID OH JLT | 36Ne 37Na run 059 |
Date: 1/04/2017
Start:16:38
BRIKEN run: 59
AIDA Run: R20_232
BigRIPS run: 214
DLT:170401_1638_Na37_059.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 17:39
BRIKEN run: 59
AIDA Run: R20_247
BigRIPS run: 0214
Root file: 170401_0157_1739_B059_Na37Ne36.root
OBSERVATIONS: |
273
|
Sat Apr 1 06:49:00 2017 |
ID,GK,JA,DK,SN,JLT | 37Na run 58 |
Date: 1/04/2017
Start:14:48
BRIKEN run: 58
AIDA Run: R20_203
BigRIPS run: 212
DLT:170401_1448_Na37_058.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 16:37
BRIKEN run: 58
AIDA Run: R20_232
BigRIPS run: 213
Root file: 170401_0157_1637_B058_Na37Ne36.root
OBSERVATIONS:
We change in the online histograms (not on the configuration file) the range of F11_PL_R,L, _HG,LG, F11RgateSiT
and the gain of F11_PL_R,l_HG,LG
15:18 No beam. Continued running.
15:23 New BigRIPS file 213
16:14 No beam. RF problems. Continued running. |
272
|
Sat Apr 1 05:01:24 2017 |
ID DK GK JLT | 36Ne 37Na run 057 |
Date: 1/04/2017
Start:13:00
BRIKEN run: 57
AIDA Run: R20_176
BigRIPS run: 210
DLT:170401_1200_Na37_057.dlt
(wrong starting time, should read 1300)
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 14:44
BRIKEN run: 57
AIDA Run: R20_203
BigRIPS run: 210
Root file:
OBSERVATIONS: spectra was NOT cleared. Some time with lower rates around 14:00 |
271
|
Sat Apr 1 04:03:31 2017 |
ID JA DK GK | Na37 Ne36 run 056 |
Date: 1/04/2017
Start:12:00
BRIKEN run: 56
AIDA Run: R20_131
BigRIPS run: 209
DLT:170401_1200_Na37_056.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 12:58
BRIKEN run: 56
AIDA Run: R20_176
BigRIPS run: 0209
Root file: 170401_0157_1159_B056_Na37Ne36.root
OBSERVATIONS: spectra was NOT cleared |
270
|
Sat Apr 1 02:07:49 2017 |
ID DK JA | Run 55 |
Date: 1/04/2017
Start:10:04
BRIKEN run: 55
AIDA Run: R20_131
BigRIPS run: 207
DLT:170401_1002_Na37_055.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 11:59
BRIKEN run: 55
AIDA Run: R20_160
BigRIPS run: 208
Root file: 170401_0157_1159_B055_Na37Ne36.root
OBSERVATIONS: 10:55 Beam stop few minutes
F11_PL_R Change the range and cleared
Two Big rips files |
269
|
Sat Apr 1 01:04:31 2017 |
ID DK JA | Na37 Ne36 Run 54 |
Date: 1/04/2017
Start: 09:03
BRIKEN run: 54
AIDA Run: R20_115903
BigRIPS run: 206
DLT: 170401_0741_Na37_053.dlt
(change name, wrong starting time) corrected to 170401_0903_Na37_054.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop:
BRIKEN run: 54
AIDA Run: R20_130
BigRIPS run: 206
Root file: 170401_0157_1004_B054_Na37Ne36.root
OBSERVATIONS: PPAC discharges every ~10min (got better) |
268
|
Sat Apr 1 00:04:10 2017 |
ID GK DK Liu | 37Na or 36Ne labels? |
The BigRIPS settings are all called "36Ne setting" but the night shift labels these runs in the BRIKEN DAQ as
"37Na". We are not sure why we label it with 37Na, we think this should be consistently named 36Ne like the
BigRIPS settings. (For sure the strongest component in the beam might be 37Na. In the 39Na settings before it
was 40Mg and we labelled it 40Mg...) |
267
|
Fri Mar 31 23:41:57 2017 |
ID, LIU, DK, GK | 37Na run 53 |
Date: 1/04/2017
Start: 07:41
BRIKEN run: 53
AIDA Run: R20_94
BigRIPS run: 205
DLT: 170401_0741_Na37_053.dlt
BRIKEN Rate: 1.5 cps
F11 Rate: 8.5 cps
Date: 1/04/2017
Stop: 09:01
BRIKEN run: 53
AIDA Run: R20_115
BigRIPS run: 205
Root file: 170401_0157_0901_B053_Na37Ne36.root
OBSERVATIONS: PPAC discharges every ~10min (got better) |
266
|
Fri Mar 31 22:45:21 2017 |
YS, LIU, DK | 37Na run 52 |
Date: 1/04/2017
Start: 06:45
BRIKEN run: 52
AIDA Run: R20_80
BigRIPS run: 204
DLT: 170401_0645_Na37_052.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 07:41
BRIKEN run: 52
AIDA Run: R20_94
BigRIPS run: 204
Root file:
OBSERVATIONS: Lots of PPAC alarms (every 5min or so) |
265
|
Fri Mar 31 22:22:40 2017 |
YS, LIU, DK | 37Na run 51 |
Date: 1/04/2017
Start: 06:23
BRIKEN run: 51
AIDA Run: R20_74
BigRIPS run: 203
DLT: 170401_0544_Na37_051.dlt
*forgot to change the time in the dlt file name
**now the file name is corrected: 170401_0623_Na37_051.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 06:43
BRIKEN run: 51
AIDA Run: R20_79
BigRIPS run: 203
Root file:
OBSERVATIONS: BigRIPS 36Ne setting with new foil |
264
|
Fri Mar 31 21:45:25 2017 |
YS, LIU, OH, DK | 37Na run 50 |
Date: 1/04/2017
Start: 05:45
BRIKEN run: 50
AIDA Run: R20_65
BigRIPS run: 202
DLT: 170401_0544_Na37_050.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 06:17
BRIKEN run: 50
AIDA Run: R20_72
BigRIPS run: 202
Root file:
OBSERVATIONS: Beam stopped at around 06:17am (BigRIPS control system crash?). |
262
|
Fri Mar 31 21:00:57 2017 |
YS, LIU, OH | 37Na run 49 |
Date: 1/04/2017
Start: 04:59
BRIKEN run: 49
AIDA Run: R20_53
BigRIPS run: 201
DLT: 170401_0459_Na37_049.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 05:44
BRIKEN run: 49
AIDA Run: R20_64
BigRIPS run: 201
Root file:
OBSERVATIONS: BigRIPS run 201 started at 04:45am. |
261
|
Fri Mar 31 20:40:47 2017 |
YS, LIU, OH | 37Na run 48 |
Date: 1/04/2017
Start: 04:38
BRIKEN run: 48
AIDA Run: R20_47
BigRIPS run: 200
DLT: 170401_0438_Na37_048.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 04:59
BRIKEN run: 48
AIDA Run: R20_52
BigRIPS run: 200
Root file:
OBSERVATIONS: At the beginning of the run the rate was low (BRIKEN 0.5cps and F11 4cps) for about 0.4x10^6 ms but it got back to around the previous value (BRIKEN 2cps and F11 8cps). |
260
|
Fri Mar 31 19:31:15 2017 |
YS, LIU, OH, CG | 37Na, run47 |
Date: 1/04/2017
Start: 03:30
BRIKEN run: 47
AIDA Run: R20_28
BigRIPS run: 199
DLT: 170401_0330_Na37_047.dlt
BRIKEN Rate: 2 cps
F11 Rate: 8 cps
Date: 1/04/2017
Stop: 04:38
BRIKEN run: 47
AIDA Run: R20_46
BigRIPS run: 199
Root file:
OBSERVATIONS: |
259
|
Fri Mar 31 18:28:54 2017 |
JLT, YS Liu, OH, CG | 37Na run 46 |
Date: 1/04/2017
Start: 02:46
BRIKEN run: 46
AIDA Run: R20_19
BigRIPS run: 198
DLT: 170401_0246_Na37_046.dlt
BRIKEN Rate: 8 cps
F11 Rate: 2 cps
Date: 1/04/2017
Stop:03:28
BRIKEN run: 46
AIDA Run: R20_28
BigRIPS run: 198
Root file:
OBSERVATIONS: We do not save the online histograms during the rest of the night shift, according to JLT's advice. |
258
|
Fri Mar 31 18:00:41 2017 |
JLT,SN,JLiu,YS,CG | 37Na run 45 |
Date: 1/04/2017
Start: 01:57
BRIKEN run: 45
AIDA Run: R20_6
BigRIPS run: 197
DLT: 170401_0157_Na37_045.dlt
BRIKEN Rate: 8 cps
F11 Rate: 1.5 cps
Date: 1/04/2017
Stop:02:25
BRIKEN run: 45
AIDA Run: R20_12
BigRIPS run: 197
Root file: 170401_0157_0225_B045_Na37.root
OBSERVATIONS: new degrader 16.8mm Al
Stopped to change stripper foil |
257
|
Fri Mar 31 16:56:16 2017 |
JLT, YS,Liu,PV,CG | New Configuration file |
New configuration file:
170331_Conf_BrikenFull.xlsx
with a new calibration
for Si_T,B and F11_PL_R,L.
Increased low energy limit for F11Rrate to 1MeV |
256
|
Fri Mar 31 15:30:24 2017 |
JLT, PV, Liu, SN, CG | 34Ne run 44 |
Date: 31/03/2017
Start: 23:27
BRIKEN run: 44
AIDA Run: R19_16
BigRIPS run: 195
DLT: 170331_2327_34Ne_044.dlt
BRIKEN Rate: 36 cps
F11 Rate: 7 cps
Date: 1/04/2017
Stop: 00:47
BRIKEN run: 44
AIDA Run: R19_37
BigRIPS run: 195
Root file: 170401_2327_0047_B044_Ne34.root
OBSERVATIONS: new degrader 16.8mm Al |
255
|
Fri Mar 31 14:40:56 2017 |
JLT, PV, Liu, CG | 34Ne run 43 |
Date: 31/03/2017
Start: 22:19
BRIKEN run: 43
AIDA Run: R19_0
BigRIPS run: 194
DLT: 170331_2219_34Ne_043.dlt
BRIKEN Rate: 38 cps
F11 Rate: 8 cps
Date: 31/03/2017
Stop: 2326
BRIKEN run: 43
AIDA Run: R19_15
BigRIPS run: 194
Root file: 170331_2219_2326_B043_Ne34.root
OBSERVATIONS: stop to change degrader from 19mm to 16.8mm |
254
|
Fri Mar 31 13:04:01 2017 |
JLT JA ID PV | 32Ne Run 42 |
Date: 31/03/2017
Start: 22:01
BRIKEN run: 42
AIDA Run: R18_000
BigRIPS run: 192
DLT: 170331_2201_32Ne_042.dlt
BRIKEN Rate: 100 cps
F11 Rate: 50 cps
Date: 31/03/2017
Stop: 22:05
BRIKEN run: 42
AIDA Run: R18_000
BigRIPS run: 192
Root file: 170331_2200_2205_B042_Ne32.root
OBSERVATIONS: |
253
|
Fri Mar 31 11:46:44 2017 |
ID PV CG | 40Mg Run 041 |
Date: 31/03/2017
Start: 19:43
BRIKEN run: 41
AIDA Run: R16_647
BigRIPS run: 186
DLT: 170331_1943_Mg40_041.dlt
BRIKEN Rate: 40/ 10= 4 cps
F11 Rate: 12 cps
Date: 31/03/2017
Stop: 20:45
BRIKEN run: 41
AIDA Run: R16_662
BigRIPS run: 186
Root file: 170331_1943_2045_B040_Mg40.root
OBSERVATIONS: |
252
|
Fri Mar 31 10:35:22 2017 |
PV CG JA | Run 40 |
Date: 31/03/2017
Start:
BRIKEN run: 40
AIDA Run: R16_630
BigRIPS run: 184
DLT: 170331_1837_Mg40_040.dlt
BRIKEN Rate: 40/ 10= 4 cps
F11 Rate: 12 cps
Date: 31/03/2017
Stop: 19:43
BRIKEN run: 040
AIDA Run: R16_647
BigRIPS run: 185
Root file: 170331_1222_1943_B040_Mg40.root
OBSERVATIONS: BigRIPS team changed to run185 after about 11min (at 18:38) |
251
|
Fri Mar 31 09:23:45 2017 |
CG PV JA | Run 39 |
Date: 31/03/2017
Start: 17:22
BRIKEN run: 039
AIDA Run: R16_611
BigRIPS run: 183
DLT: 170331_1722_Mg40_039.dlt
BRIKEN Rate: 40 cps
F11 Rate: 12 cps
Date: 31/03/2017
Stop: 18:33
BRIKEN run:39
AIDA Run: R16_628
BigRIPS run:183
Root file:170331_1222_1833_B039_Mg40.root
OBSERVATIONS: Stopped to change a stripper foil |
250
|
Fri Mar 31 08:23:32 2017 |
CG PV JA | Run 38 |
Date: 31/03/2017
Start: 16:21
BRIKEN run: 038
AIDA Run: R16_581
BigRIPS run: 182
DLT: 170331_1524_Mg40_037.dlt
BRIKEN Rate: 40 cps
F11 Rate: 12 cps
Date: 31/03/2017
Stop:
BRIKEN run: 38
AIDA Run: R16_611
BigRIPS run:182
Root file:170331_1222_1721_B038_Mg40.root
OBSERVATIONS: |
249
|
Fri Mar 31 07:17:03 2017 |
OH PV JA CG | Run 37 |
Date: 31/03/2017
Start: 15:24
BRIKEN run: 037
AIDA Run: R16_581
BigRIPS run: 181
DLT: 170331_1524_Mg40_037.dlt
BRIKEN Rate: 40 cps
F11 Rate: 12 cps
Date: 31/03/2017
Stop:
BRIKEN run: 37
AIDA Run: R16_596
BigRIPS run: 181
Root file: 170331_1222_1621_B037_Mg40.root
OBSERVATIONS: |
248
|
Fri Mar 31 05:27:44 2017 |
OH,SN,JA,PV | 40Mg run 36 |
Date: 31/03/2017
Start: 13:24
BRIKEN run: 036
AIDA Run: R16_5551
BigRIPS run: 179
DLT: 170331_1324_Mg40_036.dlt
BRIKEN Rate: 4 cps
F11 Rate: 13 cps
Date: 31/03/2017
Stop: 1324
BRIKEN run: 036
AIDA Run: R16_579
BigRIPS run: 180
Root file: 170331_1222_1514_B036_Mg40.root
OBSERVATIONS: Online cleared
BigRIPS started file 180 at 13:39 without noticing
They stop for calibration at 14:45 |
247
|
Fri Mar 31 04:57:01 2017 |
ID,YS,JLT,OH | 40Mg run 35 |
Date: 31/03/2017
Start: 12:24
BRIKEN run: 035
AIDA Run: R16_536
BigRIPS run: 178
DLT: 170331_1224_Mg40_035.dlt
BRIKEN Rate: 4 cps
F11 Rate: 13 cps
Date: 31/03/2017
Stop: 1324
BRIKEN run: 035
AIDA Run: R16_551
BigRIPS run: 178
Root file: 170331_1222_1324_B035_Mg40.root
OBSERVATIONS: Online cleared |
246
|
Fri Mar 31 03:54:26 2017 |
ID JLT | Run 034: gamma spectra background lines |
There is a strong background line at ~1293 keV. According to the attached document this could come from the
neutron activation of 115In to 116In (14s halflife) of Indium seals. |
Attachment 1: natural-gammas.pdf
|
|
245
|
Fri Mar 31 03:26:53 2017 |
ID OH SN | 40Mg Run 034 |
Date: 31/03/2017
Start: 11:23
BRIKEN run: 034
AIDA Run: R16_521
BigRIPS run: 177
DLT:170331_1123_Mg40_034.dlt
BRIKEN Rate: 4 cps
F11 Rate: 13 cps
Date: 31/03/2017
Stop: 12:24
BRIKEN run: 034
AIDA Run: R16_536
BigRIPS run: 177
Root file:170331_1123_1222_B034_Mg40.root
OBSERVATIONS: We started dividing he count rates by factor 10 (clock = 10 Hz) a few runs ago. Please check this.
Night shift has used the count rates directly from the plots. |
244
|
Fri Mar 31 02:26:19 2017 |
ID RCF | 40Mg Run 033 |
Date: 31/03/2017
Start: 10:23
BRIKEN run: 033
AIDA Run: R16_507
BigRIPS run: 176
DLT:170331_1023_Mg40_033.dlt
BRIKEN Rate: 4 cps
F11 Rate: 10 cps
Date: 31/03/2017
Stop: 11:22
BRIKEN run: 033
AIDA Run: R16_521
BigRIPS run: 176
Root file:170331_0012_1123_B033_Mg40.root
OBSERVATIONS: We started dividing he count rates by factor 10 (clock = 10 Hz) a few runs ago. Please check this.
Night shift has used the count rates directly from the plots. |
243
|
Fri Mar 31 01:50:15 2017 |
ID, RCF | 40Mg Run 032 |
Date: 31/03/2017
Start: 10:01
BRIKEN run: 032
AIDA Run: R16_502
BigRIPS run: 175
DLT:170331_1001_Mg40_032.dlt
BRIKEN Rate: 4cps
F11 Rate: 11
Date: 31/03/2017
Stop: 10:22
BRIKEN run:032
AIDA Run: R16_506
BigRIPS run: 176(beginning)
Root file:170331_0012_1022_B032_Mg40.root
OBSERVATIONS: |
242
|
Fri Mar 31 01:01:58 2017 |
ID RCF OH | Run 031 |
Date: 31/03/2017
Start: 08:58
BRIKEN run: 31
AIDA Run: R16_485
BigRIPS run: 174
DLT:170331_0858_Mg40_031.dlt
BRIKEN Rate:3.5cps
F11 Rate:11
Date: 31/03/2017
Stop: 09:44
BRIKEN run: 31
AIDA Run: R16_498
BigRIPS run: 174
Root file:170331_0012_0944_B031_Mg40.root
OBSERVATIONS:
Beam stopped at 9:44 to change the C foil |
241
|
Fri Mar 31 00:01:55 2017 |
ID JA DK GK Liu | Run 030 |
Date: 31/03/2017
Start: 07:58
BRIKEN run: 30
AIDA Run: R16_471
BigRIPS run: 173
DLT:170331_0630_Mg40_030.dlt
BRIKEN Rate:40
F11 Rate:11
Date: 31/03/2017
Stop: 8:57
BRIKEN run: 30
AIDA Run: R16_485
BigRIPS run: 173
Root file:170331_0012_0857_B030_Mg40.root
OBSERVATIONS: |
240
|
Thu Mar 30 22:19:22 2017 |
Liu DK KG JA ID | Run 28-29 |
Date: 31/03/2017
Start: 06:30
BRIKEN run: 28
AIDA Run: R16_451
BigRIPS run: 171
DLT:170331_0630_Mg40_028.dlt
BRIKEN Rate:40 divided by 10 (clock is 10Hz)
F11 Rate:11
Date: 31/03/2017
Stop: 07:57
BRIKEN run: 29
AIDA Run: R16_471
BigRIPS run: 171
Root file:170331_0012_0757_B028029_Mg40.root
OBSERVATIONS:Increase run file by accident. BigRIPS switched to 173 |
238
|
Thu Mar 30 21:01:54 2017 |
JA DK KG Liu | Run 27 |
Date: 31/03/2017
Start: 5:04
BRIKEN run: 27
AIDA Run: R16_429
BigRIPS run: 170
DLT: 170331_0503_Mg40_027.dlt
BRIKEN Rate:35
F11 Rate:12
Date: 31/03/2017
Stop: 06:17
BRIKEN run:27
AIDA Run: R16_447
BigRIPS run: 170
Root file: 170331_0012_0617_B027_Mg40.root
OBSERVATIONS: Run 26 was fake.
At 6:14 we send a clear timestamp to keep the ranges of the rates.
Beam stopped. |
237
|
Thu Mar 30 20:13:11 2017 |
JA, GK, DK | 40Mg run25 |
Date: 31/03/2017
Start: 04:13
BRIKEN run: 25
AIDA Run: R16_416
BigRIPS run: 169
DLT: 170331_0314_Mg40_025.dlt
BRIKEN Rate: 4
F11 Rate: 13
Date: 31/03/2017
Stop: 4:58
BRIKEN run: 25
AIDA Run: R16_428
BigRIPS run: 169
Root file: 170331_0012_0459_B024_Mg40.root
OBSERVATIONS: Beam stopped to change a foil |
236
|
Thu Mar 30 19:16:46 2017 |
GK,DK,JLiu,JA,JLT | 40 Mg run 24 |
Date: 31/03/2017
Start: 03:14
BRIKEN run: 24
AIDA Run: R16_402
BigRIPS run: 168
DLT: 170331_0314_Mg40_024.dlt
BRIKEN Rate: 4
F11 Rate: 13
Date: 31/03/2017
Stop: 04:10
BRIKEN run: 24
AIDA Run: R16_416
BigRIPS run: 169
Root file: 170331_0012_0409_B024_Mg40.root
OBSERVATIONS: Previous online was cleared |
235
|
Thu Mar 30 18:14:59 2017 |
JLT,DK,GK, Liu | 40Mg run23 |
Date: 31/03/2017
Start: 02:14
BRIKEN run: 23
AIDA Run: R16_387
BigRIPS run: 167
DLT: 170331_0214_Mg40_023.dlt
BRIKEN Rate: 4
F11 Rate: 13
Date: 31/03/2017
Stop: 03:14
BRIKEN run: 23
AIDA Run: R16_402
BigRIPS run: 167
Root file: 170331_0012_0314_B023_Mg40.root
OBSERVATIONS: Previous online was cleared |
234
|
Thu Mar 30 17:17:21 2017 |
JLT,GK,DK,JLiu | 40Mg run 22 |
Date: 31/03/2017
Start: 01:14
BRIKEN run: 22
AIDA Run: R16_372
BigRIPS run: 166
DLT: 170331_0012_Mg40_021.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 31/03/2017
Stop: 02:12
BRIKEN run: 22
AIDA Run: R16_387
BigRIPS run: 166
Root file:
OBSERVATIONS: Previous online was cleared
170331_0012_0212_B022_Mg40.root |
233
|
Thu Mar 30 16:15:24 2017 |
SN, JLT, GK, DK, JLiu | 40Mg run 21 |
Date: 31/03/2017
Start: 00:12
BRIKEN run: 21
AIDA Run: R16_357
BigRIPS run: 165
DLT: 170331_0012_Mg40_021.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 31/03/2017
Stop:01:14
BRIKEN run: 21
AIDA Run: R16_372
BigRIPS run: 165
Root file: 170331_0012_0114_B021_Mg40.root
OBSERVATIONS: Previous online was NOT cleared |
232
|
Thu Mar 30 13:35:30 2017 |
JLT,TD, JLiu,SN, GK | 40Mg run 20 |
Date: 30/03/2017
Start: 21:33
BRIKEN run: 20
AIDA Run: R16_318
BigRIPS run: 162
DLT:170330_2133_Mg40_020.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 31/03/2017
Stop: 00:11
BRIKEN run:20
AIDA Run: r16_357
BigRIPS run: 164
Root file: 170330_1605_0012_B020_Mg40.root
OBSERVATIONS: Previous online not cleared
START OF BIGRIPS RUN 163 AT 22:16
START OF BIGRIPS RUN 164 AT 23:07 |
Attachment 1: screenshoot_170330_2351.png
|
|
231
|
Thu Mar 30 12:27:44 2017 |
JLT,TD,JLiu,SN | 40Mg run 19 |
Date: 30/03/2017
Start: 20:26
BRIKEN run: 19
AIDA Run: R16_301
BigRIPS run: 161
DLT:170330_2026_Mg40_019.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 30/03/2017
Stop: 21:32
BRIKEN run:19
AIDA Run: r16_318
BigRIPS run: 161
Root file: 170330_1605_2132_B019_Mg40.root
OBSERVATIONS: Previous online not cleared |
230
|
Thu Mar 30 11:35:52 2017 |
JLT,TD,PV,JLiu | 40Mg run 18 |
Date: 30/03/2017
Start: 19:33
BRIKEN run: 18
AIDA Run: R16_288
BigRIPS run: 160
DLT:170330_1933_Mg40_018.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 30/03/2017
Stop: 20:25
BRIKEN run:18
AIDA Run: r16_301
BigRIPS run: 160
Root file: 170330_1605_2025_B018_Mg40.root
OBSERVATIONS: Previous online not cleared |
229
|
Thu Mar 30 10:26:06 2017 |
JLT,TD,PV | 40Mg run 17 |
Date: 30/03/2017
Start: 18:24
BRIKEN run: 17
AIDA Run: R16_270
BigRIPS run: 159
DLT:170330_1824_Mg40_017.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 30/03/2017
Stop: 19:32
BRIKEN run:17
AIDA Run: r16_288
BigRIPS run: 159
Root file: 170330_1605_1932_B017_Mg40.root
OBSERVATIONS: Previous online not cleared |
228
|
Thu Mar 30 09:24:45 2017 |
JLT,RC,TD,PV,SN | 40Mg run 16 |
Date: 30/03/2017
Start: 17:22
BRIKEN run: 16
AIDA Run: R16_252
BigRIPS run: 158
DLT:170330_1722_Mg40_016.dlt
BRIKEN Rate: 3
F11 Rate: 13
Date: 30/03/2017
Stop: 18:22
BRIKEN run:16
AIDA Run: r16_270
BigRIPS run: 158
Root file: 170330_1605_1822_B016_Mg40.root
OBSERVATIONS: Previous online not cleared |
227
|
Thu Mar 30 07:41:58 2017 |
RCF PV SN CG JA | Run 15 |
Date: 30/03/2017
Start: 16:05
BRIKEN run: 15
AIDA Run: R16_231
BigRIPS run: 157
DLT:170330_1605_Mg40_015.dlt
BRIKEN Rate: 4
F11 Rate: 13
Date: 30/03/2017
Stop: 17:21
BRIKEN run:15
AIDA Run: r16_252
BigRIPS run: 157
Root file:170330_1605_1721_B015_Mg40.root
OBSERVATIONS: |
226
|
Thu Mar 30 07:31:09 2017 |
SN PV CG RCF JA | Run 14 |
Date: 30/03/2017
Start: 15:30
BRIKEN run: 013
AIDA Run: RR16_222
BigRIPS run: run156
DLT: 170330_1528_Mg40_014.dlt
BRIKEN Rate: 3 cps
F11 Rate: 12 cps
Date: 30/03/2017
Stop: 15:39
BRIKEN run:14
AIDA Run: R16_225
BigRIPS run: 156
Root file: 170330_1528_1535_B014_Mg40.root
OBSERVATIONS: NEW DEGRADER THICKNESS 8mm (before was 11mm)
Beam stopped for a problem in a magnet. |
225
|
Thu Mar 30 06:30:06 2017 |
JA CG PV SN | Run 13 |
Date: 30/03/2017
Start: 14:25
BRIKEN run: 013
AIDA Run: R16_205
BigRIPS run: run155
DLT:170330_1426_Mg40_013.dlt
BRIKEN Rate: 40 cps
F11 Rate: 14 cps
Date: 30/03/2017
Stop: 15:25
BRIKEN run:13
AIDA Run: R16_222
BigRIPS run: 155
Root file:170330_0947_1528_B013_Mg40.root
OBSERVATIONS: |
224
|
Thu Mar 30 05:56:28 2017 |
JLT,JA,CG,PV | 40Mg Run 12 |
Date: 30/03/2017
Start: 13:54
BRIKEN run: 012
AIDA Run: R16_1196
BigRIPS run: run153
DLT: 170330_1355_Mg40_012.dlt
BRIKEN Rate: 45 cps
F11 Rate: 14 cps
Date: 30/03/2017
Stop: 14:25
BRIKEN run:12
AIDA Run: r16_205
BigRIPS run: 154
Root file:170330_0947_1425_B011_Mg40.root
OBSERVATIONS: Previous online spectra not cleared
THERE WAS SOME CONFUSION AND A NEW BRIKEN RUN WAS STARTED
BUT BIGRIPS HAD NOT STOP
NEW RUN 154 started at 14:05 |
223
|
Thu Mar 30 04:49:52 2017 |
JLT,TD | 40Mg Run 11 |
Date: 30/03/2017
Start: 12:47
BRIKEN run: 011
AIDA Run: R16_178
BigRIPS run: run153
DLT: 170330_1247_Mg40_011.dlt
BRIKEN Rate: 3 cps
F11 Rate: 11 cps
Date: 30/03/2017
Stop: 13:54
BRIKEN run: 011
AIDA Run: R16_196
BigRIPS run: 153
Root file:170330_0947_1354_B011_Mg40.root
OBSERVATIONS: Previous online spectra not cleared |
222
|
Thu Mar 30 03:55:42 2017 |
J. Agramunt | 40Mg Run 10 |
Date: 30/03/2017
Start: 11:52
BRIKEN run: 010
AIDA Run: R16_163
BigRIPS run: run152
DLT: 170330_1152_Mg40_010.dlt
BRIKEN Rate: 4 cps
F11 Rate: 12 cps
Date: 30/03/2017
Stop: 12:47
BRIKEN run: 010
AIDA Run: R16_178
BigRIPS run: 152
Root file:170330_0947_1247_B010_Mg40.root
OBSERVATIONS: |
221
|
Thu Mar 30 01:46:30 2017 |
J.Agramunt | 40Mg Run 009 |
Date: 30/03/2017
Start: 09:47
BRIKEN run: 009
AIDA Run: R16_126
BigRIPS run: run150
DLT: 170330_0948_Mg40_009.dlt
BRIKEN Rate: 4 cps
F11 Rate: 12 cps
Date: 30/03/2017
Stop: 11:51
BRIKEN run: 9
AIDA Run:R16_163
BigRIPS run: 151
Root file:170330_0947_1151_B009_Mg40.root
OBSERVATIONS:
Two BigRips files |
220
|
Thu Mar 30 00:47:04 2017 |
J. Agramunt | 40Mg Run 008 |
Date: 30/03/2017
Start: 08:41
BRIKEN run: 008
AIDA Run: R16_107
BigRIPS run: 149
DLT: 170330_0718_Mg40_008.dlt
BRIKEN Rate: 3.5 cps
F11 Rate: 12
Date: 30/03/2017
Stop: 09:46
BRIKEN run: 008
AIDA Run: R16_126
BigRIPS run: 149
Root file:170330_0840_0946_B008_Mg40.root
OBSERVATIONS: |
219
|
Wed Mar 29 22:53:58 2017 |
J. Agramunt | 40Mg Run007 |
Date: 30/03/2017
Start: 07:18
BRIKEN run: 007
AIDA Run: R16_81
BigRIPS run: 148
DLT: 170330_0718_Mg40_007.dlt
BRIKEN Rate: 3cps
F11 Rate: 13
Date: 30/03/2017
Stop: 170330_0718_840_B007_Mg40.root
BRIKEN run:007
AIDA Run:R107
BigRIPS run:148
Root file: 170330_0718_840_B007_Mg40.root
OBSERVATIONS:
Sync ok |
218
|
Wed Mar 29 21:34:20 2017 |
RCF | 40Mg Run 006 |
Date: 30/03/2017
Start: 05:42
BRIKEN run: 006
AIDA Run: R16_57
BigRIPS run: 147
DLT: 170330_0542_Mg40_006.dlt
BRIKEN Rate: 3.5cps
F11 Rate: 12
Date: 30/03/2017
Stop: 06:43
BRIKEN run:006
AIDA Run:R16_73
BigRIPS run:147
Root file:170330_0429_0643_B006_Mg40.root (accumulated)
OBSERVATIONS:
Carbon foil changed at the beginning of this run.
AIDA is still seeing "nothing" Liu changes the distance of the Al degrader from 13mm to 11mm.
Syncronization: Difference of timestamps between AIDA and BIGRIPS observed on terminals remains constant.
6:40: BIGRIPS stop the run and they ar doing calibrations for 20-30 minutes. |
217
|
Wed Mar 29 20:27:53 2017 |
RCF | 40Mg Run005 |
Date: 30/03/2017
Start: 04:29
BRIKEN run: 005
AIDA Run: R16_38
BigRIPS run: 146
DLT: 170330_0429_Mg40_005.dlt
BRIKEN Rate: 3.5cps
F11 Rate: 13
Date: 30/03/2017
Stop: 05:31
BRIKEN run:005
AIDA Run:R16_54
BigRIPS run:146
Root file:170330_0429_0531_B005_Mg40.root
OBSERVATIONS:
04:29 -> Beginning of the run Shunji and Liu removed the degrader. For this reason I erased the online
histograms from previous runs.
04:50 -> It looks like AIDA is still seeing "nothing". Shunji and Liu put the degrader back again at 13mm Al deg.
During the run: Syncronization: Difference of timestamps between AIDA and BIGRIPS observed on terminals constant. |
216
|
Wed Mar 29 19:31:21 2017 |
RCF | 40Mg Run 004 |
Date: 30/03/2017
Start: 03:29
BRIKEN run: 004
AIDA Run: R16_22
BigRIPS run: 145
DLT: 170330_0329_Mg40_004.dlt
BRIKEN Rate: 3.5cps
F11 Rate: 13
Date: 30/03/2017
Stop: 04:25
BRIKEN run:004
AIDA Run:R16_37
BigRIPS run:145
Online not erased.
Root file:170330_0216_0425_B004_Mg40.root (accumulated with previous root)
Syncronization: Difference of timestamps seems to be constant between AIDA and BIGRIPS values observed on terminals |
215
|
Wed Mar 29 18:42:25 2017 |
RCF | 40Mg Run 003 |
Date: 30/03/2017
Start: 02:39
BRIKEN run: 003
AIDA Run: R16_5
BigRIPS run: 144
DLT: 170330_0239_Mg40_003.dlt
BRIKEN Rate: 4cps
F11 Rate: 12
(First part of the run in the rate histogram was overlapping the previous data. The reason is not understood).
Date: 30/03/2017
Stop: 03:27
BRIKEN run:003
AIDA Run:R16_21
BigRIPS run:145 (just started)
Online not erased.
Root file:170330_0216_0326_B003_Mg40.root (accumulated with previous root)
Syncronization terminals on screenshots to compare with previous run. Due to the updates on each terminal are not with the same frequency it is hard to observe in the screenshots, but on live seems to be constant. |
Attachment 1: 201703300252-SyncScreenshot.png
|
|
Attachment 2: 201703300307-SyncScreenshot.png
|
|
214
|
Wed Mar 29 18:16:58 2017 |
RCF | 40Mg Run 002 |
Date: 30/03/2017
Start: 02:16
BRIKEN run: 002
AIDA Run: R16_4
BigRIPS run: 143
DLT: 170330_0216_Mg40_002.dlt
BRIKEN Rate: 6cps
F11 Rate: 13
Date: 30/03/2017
Stop: 02:38 (bigrips started new file 15 minutes ago)
BRIKEN run:002
AIDA Run:R16_5
BigRIPS run:144
Online not erased since JL left. Just Start File.
Root file: HISTOGRAMS NOT SAVED FOR THIS RUN
Observation: AIDA recovered at 02:15
Synchronization plot not generated. Some screenshots rom terminals attached. AIDA terminal has additional messages and between both terminals (AIDA/BIGRIPS) there is a constant offset apparently. |
Attachment 1: 201703300234-SyncScreenshot.png
|
|
213
|
Wed Mar 29 17:15:21 2017 |
JLT | New Config file |
New configuration file:
170330_Conf_BrikenFull.xlsx
Tha gain of F11_PL TFA was changed from x2 to x4
In Conf file histogram ranges were changed for
F11_PL_L and _R: 30 MeV
F11_PL_L_HG and _R_HG: 200 MeV
Si_T and _B: 200 MeV
the gain for F11_PL_* was changed to 0.0025 (x2)
Thhe gain for Si_* was changed to 0.0007 (x10)
A new gated spectrum was added: F11RgateSiT |
212
|
Wed Mar 29 15:16:17 2017 |
Many | 40Mg Run 001 |
Date: 29/03/2017
Start: 23:13
BRIKEN run: 1
AIDA Run: R13_36
BigRIPS run: 141
DLT: 170329_2213_Mg40_001.dlt
BRIKEN Rate: 6cps
F11 Rate: ?
Date: 30/03/2017
Stop: 00:18
BRIKEN run:001
AIDA Run:R13_52
BigRIPS run:141
Previous online not erased
Root file:170329_2213_0018_B001_Mg40.root
Observation: AIDA crash at 23:59 |
211
|
Wed Mar 29 14:14:58 2017 |
Many | 40Mg RUN 000 |
Date: 29/03/2017
Start: 22:13
BRIKEN run: 0
AIDA Run: R13_18
BigRIPS run: 140
DLT: 170329_2213_Mg40_000.dlt
BRIKEN Rate: 6cps
F11 Rate:
Stop: 23:10
BRIKEN run: 0
AIDA Run: R13_35
BigRIPS run: 140
Root file: 170329_2213_2310_B000_Mg40.root
Observations:
- We should increase the gain of F11 plastic (now a bit to small)
say by a factor of 2. Calibration is probably wrong!? |
210
|
Wed Mar 29 13:31:37 2017 |
J Agramunt, R. Caballero, T. Davinson, C. Griffin, O. Hall, D. Kahl, G. Kiss, J. Liu, S. Nishimura, V. Phong, JL Tain | Start of parasitic |
Start of parasitic Ca beam
(main experiment "New isotope search", Ahn et al.)
New directory: /data/1703Ahn/
Configuration file: 170329_Conf_BrikenFull.xlsx |
Attachment 1: 170329_Conf_BrikenFull.xlsx
|
209
|
Wed Mar 29 11:02:40 2017 |
PV, Liu, JA, JLT | F11 plastic |
New calibration of F11 plastic
We decided to have both a low gain and a high gain
for F11 plastic dividing the signal from the TFA
with a "T" and using in one branch a 20db attenuator (reduction by 10)
and sending to two different DACQ channels.
The gain of the TFA was also reduced to x2
V1A7C3: F11_PL_R (Low gain: ~60MeV)
V1A7C4: F11_PL_L
V1A7C5: F11_PL_R_HG (High gain: ~600MeV)
V1A7C5: F11_PL_L_HG |
208
|
Wed Mar 29 07:34:16 2017 |
J. Agramunt | BrikenTools repository installed at d05 |
The last version of Briken tools repository has ben installed at d05, this repository includes the Merger and the BrikenOffline codes, as well as a CommonTools folder to share scripts and code.
For update versions, just type in the desired directory "svn update". |
207
|
Wed Mar 29 03:02:02 2017 |
J. Agramunt | Synchronization test procedure (update) |
To Launch the processes:
Open 4 terminals:
Terminal 1 (DataSink) type:
>ssh aida@d05
>cd /home/aida/DataPackage/DataSink/Linux64
>DataSink -i 3
Terminal 2 (SynCheck) type:
>ssh aida@d05
>cd /home/aida/SyncCheck
>./SynCheck
Terminal 3 (BigRIPS Data Relay) type:
>ssh aida@d05
>cd /home/aida/ribfts/ribftssender
>./ribftssender_mar17ca debug
(specific for current 40Ca parasitic run because we are not sending
a pulse signal to BigRIPS as trigger but receiving triggers from
BigRIPS to create the pulses)
Terminal 4 (AIDA Data Relay) type:
>npg@aidas1
>DataRelayFilter -n 10.32.0.12 -p 10307 -I 2
"-I 2" selects ID 2 as the one for the AIDA data stream,
which must correspond to the one expected by the DataSink in the d05 PC.
The programming transmitting the data from AIDA to the DataSink includes an
intermediate filtering step. This selects only correlation scalers from one
module (and possibly ADC values from one channel in that module).
Gasific MainWindow (Briken Data Relay):
In the DAQ Control tab: Click "Start Sync Monitoring" button.
In the pop up window set server ip and port (ip:10.32.0.12, port:10305)
By default this perform a check on the differences RIBF-BRIKEN and AIDA-BRIKEN.
In case that BRIKEN is not running, the option "SynCheck -M 1" check the differences
AIDA-RIBF and BRIKEN-RIBF, while "SynCheck -M 2" checks RIBF-AIDA and BRIKEN-AIDA
To synchronize:
In the Gasific MainWindow, DAQ Control tab: Click "Send Sync Pulse" button |
206
|
Tue Mar 28 17:02:19 2017 |
DK | Applying Biases |
Today, Gabor and I discussed with Nathan from ORNL about the biasing system used for Ge, 3He, Plastic, and others. Phong is also a bit familiar with the system (edit also
Shintaro
Go). While there
is supposed to be a manual, Gabor and I did not find it.
In case of trouble: contact Nathan Brewer Gmail: Brewer.nathant@gmail.com Skype: nathan.t.brewer
Log in to high voltage PC:
$ ssh -Y pixie16@10.32.6.161
passwd: ************
For HV readout, run firefox in the background
$ firefox &
You can probably check the history or restore pages, but it should be pointed
at 192.168.13.239
It updates automatically every several seconds. Unless the HV monitor is
running, it may show nothing...
For temperatures:
$ cd ~/DAQ_1/kelvin
$ ./kelvin-read
(there are options to kill all temperatures)
For applying existing HVs (BE CAREFUL!)
$ cd ~/DAQ_1/hv-mpod
$ ./hvmon
If you want to change the voltages (up or down) kill this with Ctrl+C
To alter bias values or change which ones are on, you can edit the file:
$ ~/DAQ_1/include/hvmon.conf
Once the file is saved, restart hvmon.
We are running the above in a GNU screen session, with firefox on one computer. It has a note taped to it. Please don't use this computer for other purposes unless necessary!
Let me note that the PC we log in through has essentially no .screenrc file so you can barely understand you are actually using screen. If you are not very familiar with
screen, better not to touch it. I will put a better .screenrc later (but I also don't want to change the setup now).
28 Mar 2017 15:47:31
Ge voltage application
LN2 filling was done yesterday before lunch
D is the beam left side Ge
MPOD name
U300 D4K
U301 D4R
U302 D4G
U303 D4B
83.7 K, with 300 V
G is the beam right side Ge
MPOD name
U304 G7K
U305 G7R
U306 G7G
U307 G7B
79.6 K with 250 V (except G7R at 300 V)
All analog signals are seen in the oscilloscope with reasonable behavior
28 Mar 2017 15:56:03
Ramp up all Ge clovers.
D at 3000 V for all
G at 2500 V for all (except G7R is 3000)
28 Mar 2017 16:26:39
Biases are all applied (maybe several minutes earlier)
D4 temp 83.7 K
G7 temp 79.6 K
28 Mar 2017 17:51:09
Now we ramp up 3He and plastics. We keep the Ge on during this time.
D4 83.7 K
G7 79.6 K
Everything looks good! |
205
|
Tue Mar 28 09:10:09 2017 |
Many | 152Eu |
152Eu source inside BRIKEN for CLOVER calibration.
Also calibration of Si-dE with 60Co source
and AIDA_PL calibration with 60Co source.
File: 170328_1707_152Eu_CloverCal.root
Calibration parameters in file:
170328_1707_CloverCalibration.ods
(attached) |
Attachment 1: 170328_1707_152Eu_CloverCal.root
|
Attachment 2: 170328_1707_CloverCalibration.ods
|
204
|
Tue Mar 28 06:56:15 2017 |
PV, Liu, JA, JLT | F11 Plastic |
Calibration of new F11 plastic
(see photo)
The new plastic is 1mm thick instead of 0.2mm used last year.
Dimensions:120mm x 100mm x 1mm
HV applied: -1800V
Anode signal connected to Ortec 474 TFA
Gain: 20 x minimum; Int: 200ns; Diff: 100ns; Invert
60 Co source
THIS WAS WRONG! POLARITY OF SIGNALS WAS REVERSED.
***************************************************************
*File: 170328_1507_F11PL_60Co.root
*See attached wrong picture 170328_1507_F11_PL_RandL.pdf (R:Red, L:Black)
*
*Calibration (Gain=20):
*V1C7C3_EFIR (R): Peak(<E>=1.25MeV):2077.1 -> a1=0.0006028 MeV/u
*V1C7C4_EFIR (R): Peak(<E>=1.25MeV):1924.0 -> a1=0.0006507 MeV/u
***************************************************************
CORRECT SPECTRUM:
File: 170328_1838_F11PLCal.root
Picture: 170328_1838_F11PLCal.pdf
*************************************************************
Stopping power calculation (SRIM):
50 MeV/A 40Mg: S=102*1.184=120.8 MeV/mm
100 MeV/A 40Mg: S=102*0.7129= 72.7 MeV/mm
(Later: according LISE simulations energy loss of 40Mg is 88MeV)
What is the energy loss of the "light" particles? |
Attachment 1: 170328_1507_F11_PL_RandL.pdf
|
|
Attachment 2: 170328_1838_F11PLCal.pdf
|
|
Attachment 3: NewF11Plastic.jpg
|
|
203
|
Mon Mar 27 11:53:15 2017 |
PV,Liu | Turn on dE detector |
We applied a bias voltage of 100 V to the dE detector
Current read = 0.660 uA
compare with https://elog.ph.ed.ac.uk/BRIKEN/190. it is slighly lower.
Attachment 1-2: signal and noise level from Co60 source for the dE top
Attachment 3-4: signal and noise level from Co60 source for the dE bottom
|
Attachment 1: 1_top_60co.png
|
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Attachment 2: 2_top_noiselvl.png
|
|
Attachment 3: 3_bottom_60co.png
|
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Attachment 4: 4_bottom_noiselvl.png
|
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202
|
Mon Mar 27 09:32:55 2017 |
JLT JA CG OH DK TD RC VP GK LJ SN | 252Cf |
252Cf at the center for BRIKEN calibration
Start: 17:31
Stop: 18:00
File: 170327_1800_252Cf.root
3He tube calibration done with script BrikenCal.cpp
Result stored in 170327_1800_252Cf_Cal.ods (attached)
After visual superposition of all spectra we decided
to change only the parameters of He003 and He133
in the new calibration file. |
Attachment 1: 170327_1800_252Cf.pdf
|
|
Attachment 2: 170327_1800_252Cf.root
|
Attachment 3: 170327_1800_252Cf_Cal.ods
|
201
|
Mon Mar 27 03:50:13 2017 |
JLT JA CG OH DK TD RC VP SN | Background |
Background measurement while they play with the beam.
Start: 11:40
Stop: 16:40
File: 170327_1640_Background.root
There seems to be a second component of noise or background
above 50keV which was not there yesterday.
Beam related? |
Attachment 1: 170327_1640_Background.pdf
|
|
200
|
Sat Mar 25 13:42:23 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura, R. Caballero | Background |
BRIKEN system powered and DACQ started after movement.
All looks fine.
Background measurement:
Start: aprox 12:00
Stop: 22:24
File: 170325_2224_Background.root |
Attachment 1: 170325_2224_Background.pdf
|
|
199
|
Sat Mar 25 13:33:12 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura, R. Caballero | BRIKEN+AIDA relocated |
We moved AIDA+BRIKEN by 107cm upstream.
See attached photos.
BRIKEN was aligned with the laser and
AIDA aligned to BRIKEN. |
Attachment 1: NewLocation1.jpg
|
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Attachment 2: NewLocation2.jpg
|
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198
|
Fri Mar 24 03:28:39 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura | Background |
Background measurement overnight
Start: 19:45
Stop: 10:40
File: 170324_1040_BackgroundOvernight.root |
Attachment 1: 170324_1040_BackgroundOvernight.pdf
|
|
197
|
Thu Mar 23 10:03:51 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura | 252Cf |
252Cf source at the center for calibration
23/03/2017
Start: 19:02
Stop: 19:38
Root file: 170323_1902_1938_252Cf.root |
Attachment 1: 170323_1902_1938_252Cf.pdf
|
|
195
|
Thu Mar 23 09:30:58 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura | Power-up and 1st spectrum |
Crates powered up.
DACQ started.
New directory: /data/1703Preparation/
DACQ configuration file: 170323Conf_BrikenFull.xlsx
(copied from from 161125Conf_BrikenFull_23.16.xlsx)
Short background run: 170323_1841_Background.root.
Neutron spectrum looks OK (see attached graph)
All the tubes look Ok. |
Attachment 1: 170323_1841Background.pdf
|
|
194
|
Thu Mar 23 09:04:38 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura | Remove EURICA rails |
We remove partially the floor rails of EURICA
to proof that it is possible to move BRIKEN + AIDA.
See attached photographs of the present status.
This will allow eventually to move both detectors by about
1 meter to have a better focus at the implantation position.
This movement could be done with a minimum of cable disconnection
using the wheels of both support tables. |
Attachment 1: Donwstream-EURICA-Rail.jpg
|
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Attachment 2: Upstream-EURICA-Rail.jpg
|
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Attachment 3: GeneralView.jpg
|
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193
|
Thu Mar 23 09:01:33 2017 |
JL Tain, J Agramunt, V. Phong, C. Griffin, O. Hall, S. Nishimura | ELOG Start Preparation |
We started the preparation of 2017 campaign |
192
|
Fri Dec 9 05:25:26 2016 |
PV | Photo and schematic drawing of the Pb shielding in front of BRIKEN during Fallon experiment |
This Pb shielding structure is right behind the variable degrader |
Attachment 1: Schematic_PbShielding_FallonRun.pdf
|
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Attachment 2: IMG_1414.JPG
|
|
191
|
Thu Dec 8 04:17:49 2016 |
PV | Installing BRIKEN ELOG 2016 in RIBF local network to a personal computer |
All the RIBF123 elog website (including Takechi and Fallon experiment) can be downloaded and installed from the following link:
https://drive.google.com/file/d/0B5rBCXKaAWNARVViSTBNSE80RzQ/view?usp=sharing
To run and view the elog website in your local computer (tested with Centos 7, it may work with Ubuntu or any other linux distro)
- Extract the downloaded file:
tar -xvzf elogBRIKEN2016.tar.gz
- Go to the extracted directory and execute make
cd elogBRIKEN2016
make
- Run elogd service:
./elogd start
then it will display:
elogd 3.1.2 built Dec 8 2016, 13:24:26 revision bd75964
CKeditor detected
ImageMagick detected
Indexing logbooks ...
Create empty password file "logbooks/ribf.passwd"
done
Server listening on port 3333 ...
- Go to your web browser, enter
http://localhost:3333
- It will ask you to register a new elog account, fill in your prefered information
Login name: |
|
(name may not contain blanks) |
Full name: |
|
Email: |
|
Password: |
|
Retype password: |
and press Save button
- Next, it will ask you to choose which logbook you want to subcribe, in this case we should choose: RIBF123, then press Save buttom at the top left connner (see attached photo)
- The experimental log should be displayed then. Select RIBF123.
Ubuntu 16
Please, update/install the following packages:
sudo apt-get install python-pip python-dev libffi-dev libssl-dev libxml2-dev libxslt1-dev libjpeg8-dev zlib1g-dev
|
Attachment 1: Screenshot_from_2016-12-08_13-30-16.png
|
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190
|
Tue Nov 29 00:30:42 2016 |
PV,SN | Sillicon dE bias voltage increased |
We increase the bias voltage of the dE detector from 20 V to 100 V
Leakage current:
Before: ~0.590 uA
After 0.695 uA |
189
|
Mon Nov 28 16:18:07 2016 |
AE | DAQ synchronization |
Please see: https://elog.ph.ed.ac.uk/AIDA/493 |
188
|
Mon Nov 28 10:48:21 2016 |
JLT | Online analysis |
Comparison of current spectra with spectra from Takechi's run
(See attachment) |
Attachment 1: analysis-271116.pdf
|
|
187
|
Mon Nov 28 05:59:28 2016 |
briken | run |
======= START =======
Date 2016/11/28
Start time : 11:12
BRIKEN run : 056
Daq Conf. File : 161128Conf_BrikenFull.xlsx
DLT File name : 161128_1112
AIDA run : R28-0
AIDA start : 11:08
BigRIPS run : 1049
BigRIPS start : 09:15
---------------------------
Shifters: AT GK KD
======= Setup =======
Central fragment: 41Al @F8
--- Degraders ---
Fixed: 3mm Pb between Musics chambers
Included lead shieldings around the beam.
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. OUT
2. IN
3. IN
======= COMMENTS =======
09:13 Clover G7Red Plugged in again.
AIDAPL gain has been increased by SN from 900V to 1000V.
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/28
BRIKEN run :
BRIKEN stop :
ROOT online :
AIDA run :
AIDA stop :
BigRIPS RUN : |
186
|
Mon Nov 28 01:22:50 2016 |
BRIKEN collaboration | Elog RIBF123 & BigRIPS |
Full RIB123 Elog entries for Takechi && Fallon parasitic experiments
Update:03Dec16
Instructions:
1) Download RIBF123FullEntries.tar.gz-part-aa and RIBF123FullEntries.tar.gz-part-ab
2) Join and uncompress the file on the terminal:
# cat RIBF123FullEntries.tar.gz-part-*| tar xz
3) cd RIBF123FullEntries
4) Open with a Browser ELOGRIBF123_161203_2030_fullWeb.html
-----------------------------------------------------------
HTML elogs for BigRIPS are found by unziping BigRIPSRunSummary.zip and EXPDBRunSummary.zip
-----------------------------------------------------------
The full elog is also included in pdf file. See:
ElogRIBF123_161203_2030_Full_part1.pdf
ElogRIBF123_161203_2030_Full_part2.pdf |
Attachment 1: BigRIPSRunSummary.zip
|
Attachment 2: EXPDBRunSummary.zip
|
Attachment 3: RIBF123FullEntries.tar.gz-part-aa
|
Attachment 4: RIBF123FullEntries.tar.gz-part-ab
|
Attachment 5: ElogRIBF123_161203_2030_Full_part1.pdf
|
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Attachment 6: ElogRIBF123_161203_2030_Full_part2.pdf
|
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185
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Sun Nov 27 23:14:49 2016 |
BRIKEN coll | run 036 |
======= START =======
Date 2016/11/27
Start time : 19:28
BRIKEN run : 36
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161128_1928
AIDA run : R24
AIDA start : 19:28
BigRIPS run : 1034
BigRIPS start : 18:33
---------------------------
Shifters: PV, KG, TD
======= Setup =======
Central fragment: 41Al @F8
--- Degraders ---
Fixed: 3mm Pb between Veto plastics up and down + 1mm Al
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
TimeStamp has been reset two times during this run.
ERROR! Data acquisition with errors during this ring because not restarted after Liquid Nitrogen refilling.
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/27
BRIKEN run : 036
BRIKEN stop : 20:38
ROOT online : 161127_1928_036.root
AIDA run : R25_0
AIDA stop :
BigRIPS RUN : 1035 |
184
|
Sun Nov 27 11:23:54 2016 |
PV, GK, AE, TD | 40Mg. Run 35 |
======= START =======
Date 2016/11/27
Start time : 18:59
BRIKEN run : 035
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161127_1859
AIDA run : R23_0
AIDA start : 19:19
BigRIPS run : 40Mg-1034
BigRIPS start : 18:33
---------------------------
Shifters: PV, AE, GK, TD
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 1mm Al + 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
2016/11/27
19:19: There is a transient, AIDA DAQ found stopped due the incompleted LN2 filling.
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/27
BRIKEN run : 035
BRIKEN stop : 19:23
ROOT online :
AIDA run : R23_4
AIDA stop : 19:19
BigRIPS RUN : 1034 |
183
|
Sun Nov 27 11:15:42 2016 |
PV, GK, AE, TD | 40Mg. Run 34 |
======= START =======
Date 2016/11/27
Start time : 17:29
BRIKEN run : 034
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161127_1729
AIDA run : R22_2
AIDA start : 17:29
BigRIPS run : 40Mg-1033
BigRIPS start : 17:24
---------------------------
Shifters: PV, AE, GK, TD
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 1mm Al + 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
2016/11/27
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/27
BRIKEN run : 034
BRIKEN stop : 18:28
ROOT online :
AIDA run : R22_14
AIDA stop :
BigRIPS RUN : 1033 |
182
|
Sun Nov 27 11:07:02 2016 |
PV, GK, AE, TD | 40Mg. Run 33 - junk |
======= START =======
Date 2016/11/27
Start time : 17:17
BRIKEN run : 033
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161127_1717
AIDA run : R22_0
AIDA start : 17:17
BigRIPS run : 40Mg-1033 (and part of 40Mg-1032)
BigRIPS start : 17:24
---------------------------
Shifters: PV, AE, GK, TD
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 1mm Al + 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
2016/11/27
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/27
BRIKEN run : 032
BRIKEN stop : 17:15
ROOT online :
AIDA run : R22_1
AIDA stop :
BigRIPS RUN : 1033 |
181
|
Sun Nov 27 10:47:20 2016 |
PV,TD,GK | 40Mg. Run 32 |
======= START =======
Date 2016/11/27
Start time : 16:20
BRIKEN run : 032
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161127_1620
AIDA run : R21_0
AIDA start : 16:19
BigRIPS run : 40Mg-1032
BigRIPS start : 16:20
---------------------------
Shifters: PV, TD, GK
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 1mm Al + 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
2016/11/27
~16:10: Beam Off for a while, we entered F11 area and attached 1mm Al degrader to the beam hole in BRIKEN PE
shielding, then start the new run
~17:00: AIDA merger stopped
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB : Hz
AIDAPL : Hz
========= END =========
Date 2016/11/27
BRIKEN run : 032
BRIKEN stop : 17:15
ROOT online :
AIDA run : R21_8
AIDA stop : 17:04
BigRIPS RUN : 1032 |
180
|
Sun Nov 27 07:10:29 2016 |
BRIKEN colaboration | Run 31 |
======= START =======
Date 2016/11/27
Start time : 13:53
BRIKEN run : 031
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161127_1353
AIDA run : R20_0
AIDA start : 13:51
BigRIPS run : 1028
BigRIPS start : 12:32:36
---------------------------
Shifters:
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
------ Rates ------
BRIKEN : Hz
F11R : Hz
Clovers : Hz
VPLT : Hz
VPLB :
AIDAPL : Hz
========= END =========
Date 2016/11/26
BRIKEN run : 031
BRIKEN stop : 16:04
ROOT online : 161127_1353_031.root
AIDA run : R20_27
AIDA stop : 16:04
BigRIPS RUN : 1030 |
179
|
Sun Nov 27 04:38:15 2016 |
BRIKEN collaboration | Run 030 |
======= START =======
Date 2016/11/27
Start time : 10:41
BRIKEN run : 030
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161126_1041
AIDA run : R17_0
AIDA start : 10:41
BigRIPS run : 1025
BigRIPS start : 08:57:33
---------------------------
Shifters:
======= Setup =======
Central fragment: 40Mg
--- Degraders ---
Fixed: 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. IN
2. IN
3. OUT
======= COMMENTS =======
13:00 The syncro was lost. The TimeStamp was reset. We did not stop recording data. AIDA was writing
file R18_28, BRIKEN was writing file 161126_1041_030.dlt (@637MB). Notice that BRIKEN online histograms were not
reset, and the rates will not be plane.
------ Rates ------
BRIKEN : 200 Hz
F11R : 100 Hz
Clovers : 275 Hz
VPLT : 18 Hz
VPLB : 8 Hz
AIDAPL : 10 Hz
========= END =========
Date 2016/11/26
BRIKEN run : 030
BRIKEN stop : 13:26
ROOT online : 161126_1326_029_030.root
AIDA run : R28_33
AIDA stop : 13:26
BigRIPS RUN : 1028 |
178
|
Sun Nov 27 04:36:16 2016 |
BRIKEN collaboration | Run 020-023 |
======= START =======
Date 2016/11/26
Start time : 20:05
BRIKEN run : 020
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161126_2004_
AIDA run : R10-0
AIDA start : 20:05
BigRIPS run : 40Mg-1011
BigRIPS start : 19:30
---------------------------
Shifters: AT&AT, AE, GK
======= Setup =======
Central fragment: 41Al
--- Degraders ---
Fixed: 3mm Pb attached to beam hole in BRIKEN PE shielding
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. OUT
2. IN
3. IN
======= COMMENTS =======
2016/11/27
02:48 Beam Off for a while.
07:15 Two peaks appeared in the syncMonitor for Ribf-AIDA. It was after the refilling of Liquid Ni. Not clear if
the possible sync problem affected the measurements.
07:20 Beam OFF
------ Rates ------
BRIKEN : 1.90963e+02 Hz
F11R : 9.75134 Hz
Clovers : 2.03958e+02 Hz
VPLT : 1.87119e+01 Hz
VPLB : 7.76665 Hz
AIDAPL : 1.00896e+01 Hz
========= END =========
Date 2016/11/27
BRIKEN run : 023
BRIKEN stop : 06:25
ROOT online : 161126_2004_020_023.root
AIDA run : R10-211
AIDA stop : 06:25
BigRIPS RUN : 1022 |
177
|
Sat Nov 26 20:50:13 2016 |
GK, AT&AT | run 16-19 |
======= START =======
Date 2016/11/26
Start time : 17:21
BRIKEN run : 016
Daq Conf. File : 161125Conf_BrikenFull.xlsx
DLT File name : 161126_1721_016
AIDA run : R9-24
AIDA start : 16:35
BigRIPS run : 40Mg-1009
BigRIPS start :
---------------------------
Shifters: GK, AT&AT
======= Setup =======
Central fragment: 41Al
--- Degraders ---
Fixed: 3mm Pb between Musics
Variable:
1=(0.5mm W+1mm Al), 2=(0.3mm W+1mm Al), 3=(1mm W +1mm Al)
1. OUT
2. IN
3. IN
======= COMMENTS =======
High gamma counting is affecting rings 1-4. (gammas in beam!?)
------ Rates ------
BRIKEN : 1.12118e+02 cps
F11R : 6.26962 cps
Clovers : 1.72406e+04 cps
VPLT : 1.82165e+01 cps
VPLB : 9.08055 cps
AIDAPL : 7.42954 cps
========= END =========
Date 2016/11/26
BRIKEN run : 019
BRIKEN stop : 18:04
ROOT online : 161126_1823_016_019.root
AIDA run : R9-43
AIDA stop : 18:12
BigRIPS RUN : |
Attachment 1: 161126_1823_016_019_Rates.png
|
|
Attachment 2: 161126_1823_016_019_Rings.png
|
|
176
|
Sat Nov 26 20:48:16 2016 |
BRIKEN collaboration | run |
===== Start of measurements 41Al ====== |
175
|
Sat Nov 26 16:54:17 2016 |
AT & AT | Clovers |
Calibration of clovers |
174
|
Sat Nov 26 16:21:08 2016 |
Briken collaboration | 41Al run 2-15 |
13:08 Beam is still OFF. Background acquisition is started.
Degrader:
3 mm Pb ONLY!
13:25 Signal cables for clover G7 are connected, now G7 spectra are visible in ONLINE.
13:35 Beam Off!
14:00 Beam ON
15:08 Beam OFF, still problems with beam!
15:11 Beam ON
15:18 Acquisition is stopped. Files
161126_1308_002.dlt to 161126_1308_015.dlt
161126_1308_002.root (online)
Rates:
F11R : 4.2 & 1.0 & 9.3 Hz
BRIKEN : 150 & 12.9 & 160 Hz |
173
|
Sat Nov 26 09:31:05 2016 |
Gabor Kiss, Ariel Tarifeno, Alvaro Tolosa | Output signals from G7Red |
Preamplifier of crystal G7Red was replaced.
Output signals from G7Red are weird.
Several screen-shots of the signal are attached. The time calibration factor is 20ns/sample. |
Attachment 1: G7red_01.svg
|
|
Attachment 2: 02.svg
|
|
Attachment 3: 03.svg
|
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Attachment 4: 06.svg
|
|
172
|
Sat Nov 26 06:37:37 2016 |
AT | 41Al run 1 |
11:07 New acquisition is started for tungsten degraders
1mm W + 1mm Al
0.5mm W + 1mm Al
3mm Pb (fixed on the beam)
11:14 Online is saved and then cleared
file: 161126_1107_001_1114.root
Rates:
F11R : 10.5Hz
BRIKEN : 170 Hz
11:18 Tungsten degraders are removed.
11:20 Beam Off
11:30 Beam ON
OBS: Something happens in between with the beam intensity!!!
Rates:
F11R : 10.5Hz && 4.54 Hz
BRIKEN : 177.7 Hz && 160 Hz
11:41 Beam OFF
11:55 Acquisition is stopped. Files
161126_1107_001.dlt (full run)
161126_1107_001.root (Online from 11:18) |
171
|
Sat Nov 26 06:30:30 2016 |
AT | Setup |
Setup for parasitic experiments
Energy 41Al @ F11 is around 145MeV/u
Degraders:
- Pb 3mm width ---> IN beam
- Tungsten:
1) 0.5 mm W + 1mm Al ---> IN/OUT beam
2) 0.3 mm W + 1mm Al ---> IN/OUT beam
3) 1.0 mm W + 1mm Al ---> IN/OUT beam |
170
|
Sat Nov 26 00:15:12 2016 |
AT | 41Al run0 |
08:15 BigRips tunning for centering 41Al. Adqusition started.
Degrader: 5mm Pb located between MUSIC chambers
08:45
Beam Off for intervention
08:50
Degrader is modified to 3mm Pb
09:44
Acquisition is stopped Files:
161126_0815_000.dlt
161126_0815_000.root
Rates:
BRIKEN : 85.2 Hz
F11R : 33.5 Hz
Daq Conf. File : 161125Conf_BrikenFull.xlsx |
Attachment 1: 161126_0815_000_RateBRIKEN.svg
|
|
169
|
Sat Nov 26 00:04:15 2016 |
AT | Elog |
RIKEN Elog during Fallon Parasitic experiments
Fallon Group:
Elog is found in http://ribf-exp.riken.jp/elog/DALI2+Fall+2016/
BRIKEN collaboration:
We keep elog from Takeshi experiments (Nishimura-san desicion!). This elog is found in
http://ribf-exp.riken.jp/elog/RIBF123/ |
168
|
Fri Nov 25 23:18:04 2016 |
BRIKEN collaboration | Fallon Parasitic experiments |
===== START OF PARASITIC EXPERIMENTS ====== |
167
|
Fri Nov 25 21:50:42 2016 |
AT | New Conf File |
161125Conf_BrikenFull.xlsx |
166
|
Fri Nov 25 21:49:36 2016 |
AT | Background Beam OFF |
21:27 Beam off. Background is started.
22:10 Acquisition is stopped. Files: |
165
|
Fri Nov 25 21:48:49 2016 |
AT | DACQ |
19:00 Test calibration |
164
|
Fri Nov 25 21:47:05 2016 |
AT | Background Beam OFF |
16:17 Background beam OFF
16:27 Beam On. Acquisition stopped just after beam ON. File:
161125_1617_017.dlt
161125_1617_017.root
BRIKEN rate beam OFF (background): 0.34 +- 0.03 n/s |
Attachment 1: 161125_1617_017_BRIKEN.svg
|
|
Attachment 2: 161125_1617_017_RateBRIKEN.svg
|
|
163
|
Fri Nov 25 03:49:44 2016 |
AT | Background Beam ON |
16/11/25 12h28min: Background measurement beam ON 19B |
162
|
Fri Nov 25 03:41:40 2016 |
AT | Run setups |
Run setups during preparation of Fallon Parasitic experiments (Kanungo experiment beam time) can be found on
http://ribfdaq/~gamma16/expdbrunsum.php
A copy of the information in this page is placed here!
According to their Setup, they are using C targets on F8 and F11. The targets can be IN/OUT. |
Attachment 1: RUNsum_kanagoda.pdf
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|
161
|
Fri Nov 25 03:37:23 2016 |
AT | Background Beam OFF/ON |
16/11/24 21h06min: Background measurement Beam OFF + Beam ON tunning and 22C
21:41 : Until now Beam OFF, BigRips team tunning the machine. An online is saved
File: 161124_2106_013.root |
Attachment 1: 161124_2106_013_BRIKEN.svg
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Attachment 2: 161124_2106_013_Rings.svg
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Attachment 3: 161124_2106_013_RateBRIKEN.svg
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160
|
Fri Nov 25 03:15:46 2016 |
AT | Background Beam ON |
16/11/24 19h38min:
Background measurement during tunning of BigRips from 27-29F to 22C is started.
Files:
161124_1938_012.dlt
161124_1938_012.root |
159
|
Thu Nov 24 14:57:55 2016 |
AT | Background Beam ON |
Starting from today 12:22, the background generated by the different setups on BigRips is monitorized.
- 30 min aprox Beam off
- 25 min aprox 29F after C target in F8
- 14 min aprox Beam Off
- 272 min aprox 27F
- 11.5 min Beam Off
- Tunning for 10Min
Adquisition is stopped at 18:22
Files:
161124_1222_010.dlt
161124_1222_011.dlt
161124_1222_010.root (online)
The RUN summary for this experiments is found in
http://ribfdaq/~gamma16/expdbrunsum.php (Access only from RIKEN) |
Attachment 1: 161124_1222_010_BRIKEN.svg
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Attachment 2: 161124_1222_010_RateBRIKEN.svg
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158
|
Thu Nov 24 14:36:27 2016 |
AT | 252Cf |
Check of calibrations and rates for neutron detectors with Conf File 161107Conf_BrikenFull.xlsx
Measurement 161122_2208_003.root has been used to check the calibrations and counting rates in the BRIKEN
detector. Condition of the measurement:
252Cf at 22.5cm from moderator, opposite sede from AIDA
RESULTS
Calibrations factors:
Calibrations of the neutron detectors are reasonable in the current conditions. A check detector by detector
(see attached file) shows that the full peak for most of the counters is around 764keV. Only 3 counters are
shifted more than 10keV:
He134 741.901
He135 750.312
He140 748.587
The impact on the counting rates would not be serious.
Counting rates (n/pulser):
#########################################
Total neutron rate: 1516.28
#########################################
BY RING:
#########################################
R1 359.057
R2 222.997
R3 386.299
R4 253.833
R5 143.434
R6 90.6357
R7 60.025
The total current counting rate is lower than rate obtained in Oct 12th (total 1550.91 n/pulser). The difference
is due mainly to a decrease in the counting rates for rings 1 to 4. |
Attachment 1: CalibrationCheck_161122.xlsx
|
157
|
Thu Nov 24 02:30:56 2016 |
CG | RIBF123R1 Local ELogs |
PDFs of the local ELog for the RIBF123R1 experiment Nov 2016 |
Attachment 1: RIBF123_Elog_1
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Attachment 2: RIBF123_Elog_2
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Attachment 3: RIBF123_Elog_3
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Attachment 4: RIBF123_Elog_4
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Attachment 5: RIBF123_Elog_5
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Attachment 6: RIBF123_Elog_6
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Attachment 7: RIBF123_Elog_7
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Attachment 8: RIBF123_Elog_8
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Attachment 9: RIBF123_Elog_9
|
156
|
Tue Nov 22 10:22:07 2016 |
PV, Liu | No current observed when turning on the HV for the D4 Clover |
19:00
We've turned on the High Voltage for the D4 Clover up to ~ 1.5 kV.
There is no current (0.0 uA) observed in all the channels (crystals) of this clover while the High Voltage is
turning up.
We have turned down the HV after that.
We've checked that the NIM crate power supply for the preamp is On and the HV and peamplifier connections for
this Clover are Ok. |
155
|
Tue Nov 22 10:17:57 2016 |
ATS, PV, LIU | 252Cf |
Measurement with 252Cf at Z=22.5cm from the moderator border, opposite side from AIDA.
Clovers and Veto detectors are turned off.
Beam is off.
Files:
161122_1820_001.dlt
161122_1820_002.dlt
161122_1820_001.root
Obs: There is a problem in the online data for this run. DAQ for VME1 do not stored data. This problems seems to
be a crash on the DAQ. I restarted the system and run again the measurement. The display for voltages has lost
connection. The channels on VME1 have been checked, no problems is observed in the waveforms.
Again, this time without observing problems:
File:
161122_2208_003.dlt
161122_2208_003.root
BRIKEN spectrum is attached for this run. Counts in the pulser are 1.123e4 |
Attachment 1: 161122_2208_003_BRIKEN.svg
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154
|
Tue Nov 22 09:26:04 2016 |
A. Tarifeno-Saldivia | Noise check |
Run for checking the noise just after turn on the crates, without high voltages on the PREAMPS.
Attached calibrated histogram for the full BRIKEN detector.
Files:
161122_1820_000.dlt
161122_1820_000.root
Pulser counts: 1.179e4 |
Attachment 1: 161122_1820_000_BRIKEN.svg
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|
153
|
Tue Nov 22 08:28:36 2016 |
A. Tarifeno-Saldivia et al | New directory and Config File |
A new directory in the IFICdaq computer has been created for the parasitic measurements during the Fallon Beam Time.
The path of the folder is:
/home/dacq/Desktop/Data/2211Fallon/
All the work during this campaign will be stored in folders inside here.
For the period before the parasitic experiments, the test and check of the detector will be stored in
/home/dacq/Desktop/Data/2211Fallon/2211FallonPreparation
The Config file for the test is:
161107Conf_BrikenFull.xlsx |
152
|
Sun Nov 20 13:02:06 2016 |
Jorge, Alavaro, Jose | DACQ |
Gasific-7.0 Short Manual (Preliminary) |
Attachment 1: Gasific70Manual.pdf
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|
151
|
Sun Nov 20 12:28:27 2016 |
Jorge, Alvaro, Jose | DACQ |
Updated run protocol |
Attachment 1: GasificShort.pdf
|
|
150
|
Fri Nov 11 08:07:18 2016 |
BCR SG NTB | BRIKEN Hit Visualization |
These are the files used to create and visualize the hit patterns of the BRIKEN detector.
There are three files needed plus one input data file. The three files are "HybridBRIKENPhysicalHistogram.hpp", "HybridBRIKENPhysicalHistogram.cpp", and "HybryidBRIKEN_Tube_Info_1.txt". These files are attached to this eLog entry.
In order to run this type in a terminal
root -l HybidBRIKENPhysicalHistogram.cpp+
The plus is important, it tells ROOT to compile this with the gcc compiler and then run that compiled version of the code. It runs slow, if at all, in the ROOT C++ interpreter CINT.
The code has been tested with ROOT v5.32 and v5.34, not version 6.
At the bottom of the HybidBRIKENPhysicalHistogram.cpp file is the "main program". In it you can set the input data file, which should be a BRIKEN online root output file, and the 3He energy cuts. It is easiest if all the files are in the same folder. If there are any questions please feel free to email B. Charles (Charlie) Rasco. |
Attachment 1: HybridBRIKENPhysicalHistogram.cpp
|
//
// HybridBRIKENPhysicalHistogram.cpp
//
//
// Created by Bertis Charles Rasco on 11/4/16.
//
//
#include "HybridBRIKENPhysicalHistogram.hpp"
#include <cmath>
#include <fstream>
#include <iostream>
#include <sstream>
#include <string>
#include <stdio.h>
//#include <stdlib.h>
#include "TH1F.h"
#include "TRandom3.h"
#include "TFile.h"
// ROOT Needs this for some reason.
HybridBRIKENHistogram::HybridBRIKENHistogram(): TH2Poly()
{
}
HybridBRIKENHistogram::HybridBRIKENHistogram( const char *name, const char *title, Double_t xlow, Double_t xup, Double_t ylow, Double_t yup ):
TH2Poly( name, title, xlow, xup, ylow, yup )
{
this->ReadinTubes();
this->FillTubeCountsRandom();
// this->SetupTubes();
// this->Draw();
}
HybridBRIKENHistogram::HybridBRIKENHistogram( const char *name, const char *title, Double_t xlow, Double_t xup, Double_t ylow, Double_t yup, TString inputFileName ):
TH2Poly( name, title, xlow, xup, ylow, yup )
{
m_InputFileName = inputFileName;
this->ReadinTubes();
this->ReadInDataFromFile();
// this->SetupTubes();
// this->Draw();
}
HybridBRIKENHistogram::~HybridBRIKENHistogram()
{
}
void HybridBRIKENHistogram::ReadinTubes( void )
{
std::ifstream file("HybridBRIKEN_Tube_Info_1.txt");
std::string str;
Int_t lineCount = 0;
Int_t tubeCount = 0;
Double_t rad;
Double_t pos[2];
Int_t tubeID;
Int_t ringID;
Char_t tubeType[20];
// std::stringstream ss;
// std::string::size_type sz;
while ( std::getline(file, str) )
{
// Process str
std::stringstream ss( str);
if( lineCount > 0 )
{
tubeType[0] = 'X';
ss >> tubeID >> tubeType >> rad >> pos[0] >> pos[1] >> ringID;
rad *= 0.5;// 2R is what is in file.
// tubeID = std::stoi( str, &sz );
if( tubeID > 0 && (tubeType[0]=='R' || tubeType[0]=='U' || tubeType[0]=='O' ) )
{
if( tubeType[0] != 'O' ) m_Tubes.push_back( new HeTube( rad, pos[0], pos[1], tubeID, ringID, tubeType ) );
else if( tubeType[0] == 'O' )
{
tubeType[1] = tubeType[4];
m_Tubes.push_back( new HeTube( rad, pos[0], pos[1], tubeID, ringID, tubeType ) );
}
tubeCount++;
}
}
// if( lineCount < 11 )
// {
// std::cout << str << std::endl;
// std::cout << tubeID << ", " << tubeType[0] << tubeType[1] << ", " << rad << ", " << pos[0] << ", " << pos[1] << ", " << ringID << std::endl;
// ss >> tubeID >> tubeType >> rad >> pos[0] >> pos[1] >> ringID;
// }
lineCount++;
}
Int_t binID;
// Double_t minX = m_Tubes[0]->pos[0] - m_Tubes[0]->radius;
// Double_t maxX = m_Tubes[0]->pos[0] + m_Tubes[0]->radius;
// Double_t minY = m_Tubes[0]->pos[1] - m_Tubes[0]->radius;
// Double_t maxY = m_Tubes[0]->pos[1] + m_Tubes[0]->radius;
// Fix
// binID = this->AddBin( minX, minY, maxX, maxY );
binID = this->AddCircularBin( 0 );
// std::cout << "X: " << this->GetNbinsX() << std::endl;
// std::cout << "Y: " << this->GetNbinsY() << std::endl;
// std::cout << "Z: " << this->GetNbinsZ() << std::endl;
// std::cout << "BinID: " << binID << std::endl;
// this->SetBinContent( binID, 9);
for( Int_t i = 1; i < (Int_t) m_Tubes.size(); i++ )
{
// minX = m_Tubes[i]->pos[0] - m_Tubes[i]->radius;
// maxX = m_Tubes[i]->pos[0] + m_Tubes[i]->radius;
// minY = m_Tubes[i]->pos[1] - m_Tubes[i]->radius;
// maxY = m_Tubes[i]->pos[1] + m_Tubes[i]->radius;
// Fix AddCircularBin
// binID = this->AddBin( minX, minY, maxX, maxY );
binID = this->AddCircularBin( i );
// std::cout << "BinID: " << binID << std::endl;
// this->SetBinContent( binID, 15 + binID * 11);
}
std::cout << "Number of Lines: " << lineCount << std::endl;// = How many tubes in total?
std::cout << "Number of Tubes: " << binID << std::endl;// = How many tubes in total?
// std::cout << "Number of Bins: " << this->GetNcells() << std::endl;// = How many tubes in total?
}
void HybridBRIKENHistogram::SetupTubes( void )
{
// 1" tubes
const Int_t maxN1 = 8;
for( Int_t i = 0; i < maxN1; i++ )
{
m_Tubes.push_back( new HeTube(0.5, 2.0 * cos( i * 6.28 / maxN1 ), 2.0 * sin(i * 6.28 / maxN1 ), i, 1, "RI" ) );
}
// 2" tube at 14" radius
const Int_t maxN = 3;
for( Int_t i = 0; i < maxN; i++ )
{
m_Tubes.push_back( new HeTube(1.0, 14.0 * cos( i * 6.28 / maxN ), 14.0 * sin(i * 6.28 / maxN ), i, 2, "O2" ) );
}
Int_t binID;
Double_t minX = m_Tubes[0]->pos[0] - m_Tubes[0]->radius;
Double_t maxX = m_Tubes[0]->pos[0] + m_Tubes[0]->radius;
Double_t minY = m_Tubes[0]->pos[1] - m_Tubes[0]->radius;
Double_t maxY = m_Tubes[0]->pos[1] + m_Tubes[0]->radius;
// Fix this
binID = this->AddBin( minX, minY, maxX, maxY );
// std::cout << binID << std::endl;
// this->SetBinContent( binID, 9);
for( Int_t i = 0; i < (Int_t) m_Tubes.size(); i++ )
{
minX = m_Tubes[i]->pos[0] - m_Tubes[i]->radius;
maxX = m_Tubes[i]->pos[0] + m_Tubes[i]->radius;
minY = m_Tubes[i]->pos[1] - m_Tubes[i]->radius;
maxY = m_Tubes[i]->pos[1] + m_Tubes[i]->radius;
// Fix this
binID = this->AddBin( minX, minY, maxX, maxY );
// std::cout << binID << std::endl;
// this->SetBinContent( binID, 15 + binID * 11);
}
}
void HybridBRIKENHistogram::ReadInDataFromFile( void )
{
const Int_t lowHeCut = 600;//20;// Cut is by bin not by energy. But for 1 keV per bin they are the same.
const Int_t highHeCut = 900;//200;// Cut is by bin not by energy. But for 1 keV per bin they are the same.
m_InputFile = new TFile( m_InputFileName );
Int_t binID;
Double_t counts;
char tempCh[20];
for( Int_t i = 0; i < m_Tubes.size(); i++ )
{
binID = i + 1;
TString histName("He");
if( binID < 10 )
{
histName.Append("00");
}
else if( binID < 100 )
{
histName.Append("0");
}
// else if( binID < 1000 )
// {
// }
// histName.Append( TString::Itoa( (Int_t) binID, 10 ) );// Works for ROOT 5.34, but not for 5.32
// itoa(binID,tempCh,10);// Does not work for 5.32 unkown if works for 5.34
sprintf (tempCh, "%d", binID);// works for 5.32
histName.Append( TString( tempCh ) );
// std::cout << histName << std::endl;
TH1F *histogram = (TH1F*)m_InputFile->Get( histName.Data() );
counts = histogram->Integral( lowHeCut, highHeCut );
this->SetBinContent( binID, counts);
}
}
void HybridBRIKENHistogram::FillTubeCountsRandom( void )
{
TRandom3 rand;
// for( Int_t i = 0; i < this->GetNbins() ; i++)
// {
// hist->Fill( rand.Uniform(1.0,140.0) );
// }
for( Int_t i = 1; i <= (Int_t) m_Tubes.size(); i++ )
{
this->SetBinContent(i, rand.Gaus(1000., 50.0) );
}
}
Int_t HybridBRIKENHistogram::AddCircularBin( Int_t tubeID )
{
Int_t binID;
Double_t r = m_Tubes[tubeID]->radius;
Double_t theta;
const Int_t N = 16;
Double_t* x;
Double_t* y;
x = new Double_t[N];
y = new Double_t[N];
for( Int_t i = 0; i < N; i++ )
{
theta = i * 2.0 * 3.1415 / N;
x[i] = m_Tubes[tubeID]->pos[0] + r * cos( theta );
y[i] = m_Tubes[tubeID]->pos[1] + r * sin( theta );
}
binID = this->AddBin( N, x, y );
// Double_t minX = m_Tubes[tubeID]->pos[0] - m_Tubes[tubeID]->radius;
// Double_t maxX = m_Tubes[tubeID]->pos[0] + m_Tubes[tubeID]->radius;
// Double_t minY = m_Tubes[tubeID]->pos[1] - m_Tubes[tubeID]->radius;
// Double_t maxY = m_Tubes[tubeID]->pos[1] + m_Tubes[tubeID]->radius;
//
////
// binID = this->AddBin( minX, minY, maxX, maxY );
return binID;
}
//***************************************************************************************
// Main Program...
void HybridBRIKENPhysicalHistogram( void )
{
Double_t halfHDPEWidth = 500.0;// mm
// TString inputFileName( "161103_1426_152Eu.root" );
// TString inputFileName( "161103_1319_252Cf.root" );
// TString inputFileName( "161107_0833_Overnight.root" );
// TString inputFileName( "161108_1609_ShortBackground.root" );
// TString inputFileName( "161013_1518_137Cs60Co.root" );
TString inputFileName( "161108_2323_717273Ni.root" );
HybridBRIKENHistogram *hist = new HybridBRIKENHistogram("hBR", "HybridBRIKEN", -halfHDPEWidth, halfHDPEWidth, -halfHDPEWidth, halfHDPEWidth, inputFileName );
// HybridBRIKENHistogram *hist = new HybridBRIKENHistogram("hBR", "HybridBRIKEN", -halfHDPEWidth, halfHDPEWidth, -halfHDPEWidth, halfHDPEWidth );
hist->Draw("COLZ");
}
|
Attachment 2: HybridBRIKENPhysicalHistogram.hpp
|
//
// HybridBRIKENPhysicalHistogram.hpp
//
//
// Created by Bertis Charles Rasco on 11/4/16.
//
//
#ifndef HybridBRIKENPhysicalHistogram_hpp
#define HybridBRIKENPhysicalHistogram_hpp
#include <vector>
#include "TFile.h"
#include "TH2Poly.h"
#include "TObject.h"
#include "TString.h"
//class TFile;
class HeTube
{
public:
HeTube( Double_t r, Double_t x, Double_t y, Int_t tID, Int_t rID, char tubeTypeChars[2] )
{ radius = r; pos[0] = x; pos[1] = y; tubeID = tID; ringID = rID;
tubeType[0] = tubeTypeChars[0]; tubeType[1] = tubeTypeChars[1]; }
//private:
Double_t radius;
Double_t pos[2];
Int_t tubeID;
Int_t ringID;
Char_t tubeType[2]; // RI (RIKEN), UP (UPC), O1 (ORNL1), O2 (ORNL2)
};
class HybridBRIKENHistogram : public TH2Poly
{
public:
HybridBRIKENHistogram();// ROOT needs this to be defined if it is inherited from a ROOT class.
HybridBRIKENHistogram( const char *name, const char *title, Double_t xlow, Double_t xup, Double_t ylow, Double_t yup );
HybridBRIKENHistogram( const char *name, const char *title, Double_t xlow, Double_t xup, Double_t ylow, Double_t yup,
TString inputFileName );
~HybridBRIKENHistogram();
ClassDef(HybridBRIKENHistogram,1);// ROOT also needs this if it is inherited from a ROOT class. Not sure what the 1 means.
private:
void ReadinTubes( void );
void SetupTubes( void );
void ReadInDataFromFile( void );
void FillTubeCountsRandom( void );
Int_t AddCircularBin( Int_t tubeID );
TString m_InputFileName;
TFile *m_InputFile;
std::vector<HeTube*> m_Tubes;
};
#endif /* HybridBRIKENPhysicalHistogram_hpp */
|
Attachment 3: HybridBRIKEN_Tube_Info_1.txt
|
ID Type 2R(mm) X(mm) Y(mm) RING
1 RIKEN 27.5 -77.45 -39.25 1
2 RIKEN 27.5 -77.45 0 1
3 RIKEN 27.5 -77.45 39.25 1
4 RIKEN 27.5 -106.052 -19.625 2
5 RIKEN 27.5 -106.052 19.625 2
6 RIKEN 27.5 -134.655 0 3
7 RIKEN 27.5 77.45 -39.25 1
8 RIKEN 27.5 77.45 0 1
9 RIKEN 27.5 77.45 39.25 1
10 RIKEN 27.5 106.052 -19.625 2
11 RIKEN 27.5 106.052 19.625 2
12 RIKEN 27.5 134.655 0 3
13 RIKEN 27.5 -177.45 -39.25 1
14 RIKEN 27.5 -177.45 0 1
15 RIKEN 27.5 -177.45 39.25 1
16 RIKEN 27.5 -206.052 -19.625 2
17 RIKEN 27.5 -206.052 19.625 2
18 RIKEN 27.5 -234.655 0 3
19 RIKEN 27.5 177.45 -39.25 1
20 RIKEN 27.5 177.45 0 1
21 RIKEN 27.5 177.45 39.25 1
22 RIKEN 27.5 206.052 -19.625 2
23 RIKEN 27.5 206.052 19.625 2
24 RIKEN 27.5 234.655 0 3
25 UPC 27.5 -118.3 77.45 3
26 UPC 27.5 -69.7 77.45 1
27 UPC 27.5 -34.85 77.45 1
28 UPC 27.5 0 77.45 1
29 UPC 27.5 34.85 77.45 1
30 UPC 27.5 69.7 77.45 1
31 UPC 27.5 118.3 77.45 3
32 UPC 27.5 -97.2 116.7 3
33 UPC 27.5 -60.362 112.3 2
34 UPC 27.5 -17.425 107.631 2
35 UPC 27.5 17.425 107.631 2
36 UPC 27.5 60.362 112.3 2
37 UPC 27.5 97.2 116.7 3
38 UPC 27.5 -73.928 151.378 3
39 UPC 27.5 -34.85 137.812 3
40 UPC 27.5 0 147.15 3
41 UPC 27.5 34.85 137.812 3
42 UPC 27.5 73.928 151.378 3
43 UPC 27.5 -27.0595 178.438 3
44 UPC 27.5 27.0595 178.438 3
45 UPC 27.5 -118.3 -77.45 3
46 UPC 27.5 -69.7 -77.45 1
47 UPC 27.5 -34.85 -77.45 1
48 UPC 27.5 0 -77.45 1
49 UPC 27.5 34.85 -77.45 1
50 UPC 27.5 69.7 -77.45 1
51 UPC 27.5 118.3 -77.45 3
52 UPC 27.5 -97.2 -116.7 3
53 UPC 27.5 -60.362 -112.3 2
54 UPC 27.5 -17.425 -107.631 2
55 UPC 27.5 17.425 -107.631 2
56 UPC 27.5 60.362 -112.3 2
57 UPC 27.5 97.2 -116.7 3
58 UPC 27.5 -73.928 -151.378 3
59 UPC 27.5 -34.85 -137.812 3
60 UPC 27.5 0 -147.15 3
61 UPC 27.5 34.85 -137.812 3
62 UPC 27.5 73.928 -151.378 3
63 UPC 27.5 -27.0595 -178.438 3
64 UPC 27.5 27.0595 -178.438 3
65 ORNL1 27.5 -215.5 77.45 5
66 ORNL1 27.5 -166.9 77.45 4
67 ORNL1 27.5 166.9 77.45 4
68 ORNL1 27.5 215.5 77.45 5
69 ORNL1 27.5 -301.012 214.133 7
70 ORNL1 27.5 -252.393 235.169 7
71 ORNL1 27.5 252.393 235.169 7
72 ORNL1 27.5 301.012 214.133 7
73 ORNL1 27.5 -215.5 -77.45 5
74 ORNL1 27.5 -166.9 -77.45 4
75 ORNL1 27.5 166.9 -77.45 4
76 ORNL1 27.5 215.5 -77.45 5
77 ORNL1 27.5 -301.012 -214.133 7
78 ORNL1 27.5 -252.393 -235.169 7
79 ORNL1 27.5 252.393 -235.169 7
80 ORNL1 27.5 301.012 -214.133 7
81 ORNL2 53 -139.932 142.007 4
82 ORNL2 53 -70.014 198.718 4
83 ORNL2 53 0 217.478 4
84 ORNL2 53 70.014 198.718 4
85 ORNL2 53 139.932 142.007 4
86 ORNL2 53 -214.903 127.3 5
87 ORNL2 53 -133.044 210.494 5
88 ORNL2 53 -48.6976 259.192 5
89 ORNL2 53 48.6976 259.192 5
90 ORNL2 53 133.044 210.494 5
91 ORNL2 53 214.903 127.3 5
92 ORNL2 53 -273.203 102.2 6
93 ORNL2 53 -263.894 172.91 6
94 ORNL2 53 -204.385 193.709 6
95 ORNL2 53 -118.139 282.073 6
96 ORNL2 53 0 313.728 6
97 ORNL2 53 118.139 282.073 6
98 ORNL2 53 204.385 193.709 6
99 ORNL2 53 263.894 172.91 6
100 ORNL2 53 273.203 102.2 6
101 ORNL2 53 -339.453 102.2 7
102 ORNL2 53 -323.857 159.305 7
103 ORNL2 53 -201.103 278.553 7
104 ORNL2 53 -166.264 365.428 7
105 ORNL2 53 -73.6089 352.162 7
106 ORNL2 53 73.6089 352.162 7
107 ORNL2 53 166.264 365.428 7
108 ORNL2 53 201.103 278.553 7
109 ORNL2 53 323.857 159.305 7
110 ORNL2 53 339.453 102.2 7
111 ORNL2 53 -139.932 -142.007 4
112 ORNL2 53 -70.014 -198.718 4
113 ORNL2 53 0 -217.478 4
114 ORNL2 53 70.014 -198.718 4
115 ORNL2 53 139.932 -142.007 4
116 ORNL2 53 -214.903 -127.3 5
117 ORNL2 53 -133.044 -210.494 5
118 ORNL2 53 -48.6976 -259.192 5
119 ORNL2 53 48.6976 -259.192 5
120 ORNL2 53 133.044 -210.494 5
121 ORNL2 53 214.903 -127.3 5
122 ORNL2 53 -273.203 -102.2 6
123 ORNL2 53 -263.894 -172.91 6
124 ORNL2 53 -204.385 -193.709 6
125 ORNL2 53 -118.139 -282.073 6
126 ORNL2 53 0 -313.728 6
127 ORNL2 53 118.139 -282.073 6
128 ORNL2 53 204.385 -193.709 6
129 ORNL2 53 263.894 -172.91 6
130 ORNL2 53 273.203 -102.2 6
131 ORNL2 53 -339.453 -102.2 7
132 ORNL2 53 -323.857 -159.305 7
133 ORNL2 53 -201.103 -278.553 7
134 ORNL2 53 -166.264 -365.428 7
135 ORNL2 53 -73.6089 -352.162 7
136 ORNL2 53 73.6089 -352.162 7
137 ORNL2 53 166.264 -365.428 7
138 ORNL2 53 201.103 -278.553 7
139 ORNL2 53 323.857 -159.305 7
140 ORNL2 53 339.453 -102.2 7
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Draft
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Thu Nov 10 05:05:54 2016 |
KM | How to convert ridf-file to root-file |
1. Login to briken@ribfana03.riken.jp
2. Check if the ridf-file you want to convert is in the directory; /home/briken16/rawdata/bigrips/
3. Login to anaroot; type "anarootlogin"
4. Make your account as your name, and create your directory.
5. login to root; "root -l"
6. root[ ] .L MakeFullBigRIPSTree_BRIKEN.C+
7. root[ ] MakeFullBigRIPSTree_BRIKEN(" full name of ridf-file ", Brho34 , Brho56 ," full name of output file ")
You can check Brho34 and Brho56 in ---> http://bripscnt01.rarfadv.riken.jp/runsum/index.php
Find the link to the summary page in the "file" column.
For example: MakeFullBigRIPSTree_BRIKEN("radiioff0371.ridf", 7.176, 6.905, "test.root")
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148
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Wed Nov 9 02:02:22 2016 |
Iris | Boron rubber from India |
The boron rubber from India is BR-2871, price US-$ 2700 for 2pc 1m x 2m x 3.3mm.
52% B content, density 1.61 g/cm3 |
Attachment 1: BPE2_Clr.jpg
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Attachment 2: quotation_220213.pdf
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Attachment 3: flex_boron_2871.pdf
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Draft
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Wed Nov 9 01:04:35 2016 |
Iris | Drawing of present setup |
This is the setup which was used for the Ni runs (from Nov. 8th evening on).
Note (Nov. 10th): Alejandro built a U-shaped Pb wall, the degrader inside AIDA was removed and possibly a Al plate was installed. This has to be checked when access is possible again.
> Attached is the present setup including all walls, auxiliary detectors, degraders etc. and the Takechi setup.
> The lead wall will be removed for measurements (of course...).
> Not to scale! Some sizes and distances included. Pictures see Jose's entry ID 110.
>
> Note the shape of the active area of the DeltaE Silicon detector, see previous entry. |
Attachment 1: Setup-161109-Takechi.pdf
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146
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Wed Nov 9 01:02:53 2016 |
Iris | Elog |
From Nov. 9th on we use the Takechi ELOG for the run information:
http://ribf-exp.riken.jp/elog/RIBF123/ |
145
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Tue Nov 8 17:00:27 2016 |
NTB, CG, AT | Si Delta E |
At least during the timeframe in between ~ 21:30 (11/08) - 23:30 (11/09) (161108_2323_717273Ni.root) we see that the silicon dE have a very low counting rate. ~1Hz when the first AIDA detector sees ~600 Hz and a cumulative ~2kHz. The energy range in the dE stops at ~10MeV.
Edit: It appears the Si dE were removed. Some signals are still in the spectra. |
144
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Tue Nov 8 15:10:24 2016 |
Many | 717273Ni Run |
F7 OUT F11 C-6mm
Start: 00:09
Run: 006
DLT: 161108_2251_717273Ni_006.dlt
Rates:
F11R: 1200 cps
BRIKEN: 270 cps (22.5%)
They were tuning during this run.
Stop: 0042
Root file: 161109_0042_717273Ni.root |
143
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Tue Nov 8 14:28:54 2016 |
Many | 717273Ni run |
F7 CH2 F11 C-6mm
Total degrader thickness 6mm
Start:
RUN: 005
File: 161108_2251_717273Ni_005.dlt
Stop: 23:59
Run: 005
Rates:
F11R: 2600 cps
BRIKEN: 740 cps
Root file: 161109_0005_717273Ni.root
Counts:
F11R: 5.36294e+06
BRIKEN: 1.42823e+06
Corr_BR_F11R: 1.41452e+06 |
142
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Tue Nov 8 13:49:58 2016 |
Many | 71,72,73Ni |
F7 CH2 F11 Empty
We remove the 8mm Al plate from inside BRIKEN infront of AIDA
Move AIDA to the central position. We put a 5mm Al plate in front
of the degrader.
Degrader 5.4mm + 5mm
Start: 22:51
DLT: 161108_2251_717273Ni_03.dlt
We remove some degrader:2.2mm off
Then we start a new run: 004
Stop:23:26
To put the C-6mm target in F11
ROOT file: 161108_2323_717273Ni.root |
141
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Tue Nov 8 12:51:08 2016 |
Many | 717273Ni |
After removing the lead wall.
Start: 21:45
DLT: 161108_2145_717273Ni_001.dlt
During the first part we were changing the degrader.
Now they remove the C-6mm target.
So we increase the adjustable degrader to 5.4mm
keeping the 8mm thick plate for implantation.
We stop and start a new DLT file at 22:02
DLT: 161108_2145_717273Ni_002.dlt
Stop: 22:48
NO ROOT FILE! |
140
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Tue Nov 8 12:30:33 2016 |
Tain, Ale (who are not on shift) | 71,72,73Ni run |
71,72,73Ni run
We started at approximately 21:00, only online, not writing on tape.
The lead is still in the way. We removed the degrader (fully) and the effect is a 5 % reduction of the neutron flux
(determined using the rate of the rateF11/rateBRIKEN before and after the change). |
139
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Tue Nov 8 11:51:28 2016 |
Ale | spikes on some spectra |
Some spectra show spikes or do not look normal. This should be checked.
Look at BRIKEN, Ring4, Ring5, Ring6, Ring7, D4, G7, Clovers,
Rate1, Rate2, Rate3, etc.
Reset time stamp: 21.00, 8th-nov.
Probably there was a problem with the clock from AIDA related to the LN2 filling.
So to recover, we need to stop acq (only stop acquisition in DACQ control),
send to hard (send parameters again) and once all the parameters were sent,
Send Sync pulse. |
138
|
Tue Nov 8 08:49:51 2016 |
Tain et al | Move ELOG |
We will start to use the internal RIKEN ELOG
It is not clear that we can keep the present ELOG also updated |
137
|
Tue Nov 8 08:31:52 2016 |
Tain et al | 424344Ca run |
Sequence of settings:
1) No target at F7 and Empty target at F11 (up to t=1E6ms)
2) No target at F7 and C-6mm target at F11 (up to t=5.1E6ms)
3) CH2 (10mm) target at F7 and C-6mm target at F11 (from t=5.3E6ms up to 6.8E6)
4) CH2 (10mm) target at F7 and Empty target at F11 (from t=6.8ms up to crash 7.1ms)
DAQ chash because start of Clover LN2 filling!
Counts accumulated in the the same time channel at the end.
Start: 16:29 Run: 000
Stop: 18:28 Run: 000
DLT filename: 161108_1629_424344Ca_000.dlt
ROOT filename: 161108_1828_424344Ca.root |
136
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Tue Nov 8 06:39:25 2016 |
Tain. Iris | Drawing of present setup |
Attached is the present setup including all walls, auxiliary detectors, degraders etc. and the Takechi setup.
The lead wall will be removed for measurements (of course...).
Not to scale! Some sizes and distances included. Pictures see Jose's entry ID 110.
Note the shape of the active area of the DeltaE Silicon detector, see previous entry. |
Attachment 1: Full_BRIKEN_Setup-includingTakechi.pdf
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135
|
Tue Nov 8 06:13:11 2016 |
Tain et al | New plastic detector in F11 |
There is a new plastic scintillator
after the MUSIC chambers
The detector has a central hole of 108mm (with) x 38mm (height)
and is 3mm thick and is placed behind the existing plastic
scintillator which is 5mm thick.
(see photo) |
Attachment 1: PlasticsBehinMUSIC1.jpg
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Attachment 2: PlasticsBehindMUSIC2.jpg
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134
|
Tue Nov 8 02:49:19 2016 |
PV, Liu | Specification of the dE silicon detector |
The specification and picture of the dE silicon detector is shown in the attached photos.
The detector has an effective area of 134 x 123 mm and 320 micrometer thick
There are 26 vertical strips. They are combined into 2 readout channels (top and bottom which respect to the orientation of the detector in BRIKEN) |
Attachment 1: spec_de_1.jpg
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Attachment 2: spec_de_2.jpg
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Attachment 3: IMG_1340.JPG
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133
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Mon Nov 7 14:17:23 2016 |
BRIKEN collaboration | Picture of shift schedule |
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Attachment 1: IMG_20161107_183105.jpg
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131
|
Mon Nov 7 13:44:26 2016 |
Alvaro, Ale, Jorge, Jose | Running Gasific and run protocol |
Preliminary |
Attachment 1: GasificShort.pdf
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130
|
Mon Nov 7 13:15:07 2016 |
Alvaro, Ale, Jorge, Jose | Background |
Background measurement overnight.
Start: 23:27 (07/11/2016)
Stop: 07:52 (08/11/2016)
ROOT file: 161108_0751_Overnight.root
The spectra have a terrible aspect!
This is consequence of DACQ crashing because LN2 filling! |
Attachment 1: 161108_0751_Overnight_BRIKEN.pdf
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129
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Mon Nov 7 13:11:42 2016 |
Alvaro, Ale, Jose, Jorge | New directory and Config file |
For second part of Takechi's run:
Directory: /data/1611Commissioning/161107Parasitic
Config File: 161107Conf_BrikenFull.xlsx |
Attachment 1: 161107Conf_BrikenFull.xlsx
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128
|
Mon Nov 7 09:05:09 2016 |
Iris | Draft for Run sheet |
Attached is the draft for the paper run sheet (version 2). If something is missing, please let me know. |
Attachment 1: Run_sheet-Nov16-v2.pdf
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Attachment 2: Run_sheet-Nov16-v2.docx
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127
|
Mon Nov 7 09:04:10 2016 |
Phong,Liu,Ale,Jose | New AIDA plastic calibration |
To have a range of about 200 MeV
Ortec671 Gain from x20 to x5 (fine gain : x0.5)
HV from 1500V to 1300V
60Co-> 10 mV
Root file: 161107_1800_AIDAplasticCalib.root
calibration a1= 0.001 MeV/units |
Attachment 1: 161107_1800_AIDAplasticCalib.pdf
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126
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Mon Nov 7 06:55:01 2016 |
NTB, SG | HPGe Fill line to D4 replaced |
HPGe fill line to D4 replaced only small leak (overflow) once Ge is full.
Solenoid was also wrapped to no effect. AIDA DAQ still stops writing.
Boron sheet and extra polyethylene were placed back on top.
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125
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Mon Nov 7 05:36:20 2016 |
Ale | new calibration for F11 |
new calibration for F11
Using a value of 70 MeV energy loss and the file 161107_0833_Overnight.root
We obtained new peak positions: for V1A7C3 peak at 5398 (F11 right), for V1A7C4 (F11 left) peak at 6060
F11_rigth (V1A7C3): 0.01297
F11_left (V1A7C4): 0.01155 |
124
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Mon Nov 7 04:49:57 2016 |
Tain, Ale | AIDA plastic (veto) and Si de calibration |
AIDA plastic (veto) and Si de calibration
For the calibration the Compton edge of the spectrum seen in the detectors was used.
There is a large uncertainty in that determination, since the spectra are not so clear in terms of shape.
For the spectra V1A7C13_EFIR (Si de, top) the channel position is 12900 units
For the spectra V1A7C14_EFIR (Si de, bottom) the channel position is 12950 units
For the spectra V1A7C9_EFIR (AIDA plastic) the channel position is 10425 units
These corresponds to the following calibration factors using 0.9 MeV as the Compton energy from Co source:
V1A7C13_EFIR (Si de, top): 6.976744E-5
V1A7C14_EFIR (Si de, bottom): 6.949807E-5
V1A7C9_EFIR (AIDA plastic): 8.633094E-5 |
123
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Mon Nov 7 04:37:33 2016 |
Phong,Liu,... | Si de and AIDA plastic calibration |
60Co source placed close to the detectors:
ROOT files:
161107_1221_SiDetCalibration.root
161107_1237_AIDAPlasticCalibration.root |
122
|
Mon Nov 7 02:39:55 2016 |
Ale | Photo of the white board with the details on the cards and preamps at B1F |
Photo of the white board with the details on the cards and preamps at B1F |
Attachment 1: New_Doc_160_2.pdf
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121
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Sun Nov 6 23:35:42 2016 |
Tain et al. | Overnight measurement: Ca isotopes |
First 50,49,48Ca beam and then 47,46,45Ca beam
C-6mm IN and OUT
New Configuration file: 161107Conf_BrikenFull.xlsx
Start: 00:43
Stop: 08:33
Tmeas:12883.1 s
ROOT file: 161107_0833_Overnight.root
There is a change of gain for F11_PL_R and F11_PL_L
Rates:
F11R: 1150 cps / 950 cps
BRIKEN: 70->40 cps / 45->25 cps
VPLT: 34->12 cps / 34->12 cps
VPLB: 6->2 cps / 6->2 cps
Counts:
RateF11R: 1.41342e+07
RateBRIKEN: 697082. (4.9 neutrons/100 particles)
Corr_BR_F11R: 632710 (91%)
Estimated background: 5153.24
RateVPLT: 376233.
Corr_BR_VPLT: 213977 (315) |
Attachment 1: 161107_0833_Overnight_Rates.pdf
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Attachment 2: 161107_0833_Overnight_F11.pdf
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Attachment 3: 161107_0833_Overnight_CorrBRF11R.pdf
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120
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Sun Nov 6 07:16:59 2016 |
Tain et al. | 58Ni on F7 CH2 F11 empty/C6mm |
CH2 target at F7 in
Start with Empty at F11
Change to C-6mm at F11 later
Start: 16:16
Stop: 17:25
Change to C-6mm at 16:47 (at 544E6 ms in Timestamp units)
ROOT file: 161106_1725_58Ni_F7CH2.root
Rates:
F11R: 2000 cps
BRIKEN: 20 cps -> 35 cps
VPLT: 16 cps -> 40 cps
VPLB: 1.5 cps -> 5.5 cps
Figures Rate BRIKEN (red) Rate V_PL_T (blue)
Counts:
RateF11R: 8006721
RateBRIKEN: 111089 (1.4 neutron/100 particles)
Corr_BR_F11R: 108817 (98%)
RateBRVPLT: 115440
Corr_BR_VPLT: 21486 (19%)
RateBRVPLB: 16109 |
Attachment 1: 161106_1725_58Ni_F7CH2_Rates.pdf
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Attachment 2: 161106_1725_58Ni_F7CH2_RatesRings.pdf
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119
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Sun Nov 6 06:39:23 2016 |
Tain et al. | 58Ni on F11 C-6mm |
58Ni in F11 C-6mm (later empty)
F7 CH2 target out (F5 CH2 target in)
Thresholds in V_PL_* lowered from 20MeV to 1MeV
Start: 15:37
Stop: 1609
ROOT file:
They put the empty position of the F11 target ladder
at 15:48.
BRIKEN neutron count rate was reduced by a factor 2!
Also veto plastic det.
Rates:
F3: 4000 cps
F11_PL_R: 1350 cps
BRIKEN: 23 cps -> 14 cps
VPLT: 28 cps -> 12 cps
VPLB: 4 cps -> 1 cps
ROOT File: 161106_1609_58Ni_F11_empty.root
Figures Rate BRIKEN (red) Rate V_PL_T (blue)
Counts:
RateF11R: 2512767
RateBRIKEN: 30363 (1.2 neutron/100 particles)
Corr_BR_F11R: 29176 (96%)
RateBRVPLT: 31275
Corr_BR_VPLT: 5424 (17%)
RateBRVPLB: 3764 |
Attachment 1: 161106_1609_58Ni_F11_empty_Rates.pdf
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118
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Sun Nov 6 06:27:49 2016 |
Tain et al. | 58Ni on F11 C-6mm in |
New calibration in V_PL_T and V_PL_R (Energyx1/2)
Start: 15:15
Stop: 15:35
File: 161106_1535_58Ni_F11_C6mm.root
Rates
F11_PL_R: 1300 cps
BRIKEN: 22 cps
V_PL_T: 7 cps
V_PL_B: 0.3 cps |
117
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Sun Nov 6 03:12:55 2016 |
Alvaro,Jorge | Overnight measurement |
Measurement during beam production
and measurement with F7 CH2 out,
F11 C-tar in/out, F7 CH2 in C-target out/in
START: 02:45
STOP: 12:47
ROOT file: 161106_1247_Overnight.root |
116
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Sat Nov 5 17:07:27 2016 |
Tain, Alvaro, Jorge | 62Ni in F7 |
62Ni beam in F7 ON CH2 target
Strat with C target ladder in F11 in empty position.
They changed to C 6mm after a while (5-10min) but we
didnt realized that!
THERE ARE NO APPRECIABLE DIFFERENCES WITH THE C-TARGET IN OR OUT!
DLT: 161106_0210_62Ni_F7_empty_002.dlt
Start: 02:10
Stop: 02:32
tlife: 1292.80 s
ROOT file: 161106_0232_62Ni_F7_empty.root
Rates at 2:19
F3: 2800 cps
F11: 1200 cps
BRIKE: 32 cps
VPLT: 17 cps
VPLR: 1 cps
Counts:
RateBRIKEN: 47703 (36.9 cps)
RateF11R: 1688270 (1305.90 cps)
Corr_BR_F11R: 47603
(all neutrons are correlated with a particle going through F11)
RateBRVPLT: 23826 (18.43 cps)
Corr_BR_VPLT: 7557
(15.8% of the neutrons are correlated with a particle
going through plastic veto top)
RateBRVPLB: 1865 (1.44 cps)
(the rate is 12.8 times smaller than top detector) |
Attachment 1: 161106_0232_62Ni_F7_empty_Rates.pdf
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Attachment 2: 161106_0232_62Ni_F7_empty_F11.pdf
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Attachment 3: 161106_0232_62Ni_F7_empty_CorrBRF11R.pdf
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Attachment 4: 161106_0232_62Ni_F7_empty_VPL.pdf
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Attachment 5: 161106_0232_62Ni_F7_empty_CorrBRVPL.pdf
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115
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Sat Nov 5 16:27:13 2016 |
Tain,Ale,Jorge,Alvaro | 62Ni beam in F11 empty target |
Empty position of the target ladder at F11
(hole is smaller than beam size)
CH2 target at F7 is OUT
DLT 161106_0126_62Ni_F11_empty_001
Start: 01:26
Stop: 01:40
NO ROOT FILE!!
At 01:32:
Rate at F3: 2600 cps
Rate at F11: 850 cps
Rate at BRIKEN: 13 n/s
Rate at VPLT: 3 cps
Rate at VPLB: 0.1 cps |
114
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Sat Nov 5 15:07:11 2016 |
Tain, Ale | 62Ni beam on F11 C-6mm |
62Ni on 6 mm C target between MUSICs
The background before was 0.36 neutrons/s
Now it is around 10 n/s
With 3100 counts/s at F3 we have of the order of 25 neutrons/s
There is an slightly higher than 10 factor between the rate of
the plastic top and bottom (13 cts/s vs 1ct/s).
Rate at F11 (plastic) 900 cts/s.
We start a proper measurement with DLT
Reset Timestamp
They will measure with 6mm C target (between MUSICS) for
about 45 minutes and then 15 min without target.
CH2 target at F7 is OUT (beam going directly to F11).
DLT: 161106_0026_62Ni_F11_C6mm_000
Run: 000
Start: 00:27
Stop: 01:17
tlife=3007 s
At 00:37
Rate at F3: 3000 cps
Rate at F11: 900 cps
Rate at BRIKEN: 25 n/s
Rate at VPLT:13 cps
Rate at VPLB: 0.8 cps
Root File: 161106_0117_62Ni_F11_C6mm.root
Figure with rates: F11 (black), BRIKEN (red), Clovers (green)
V_PL_T (blue), V_PL_B (pink)
Figure with F11 spectra: Right (red), Left (blue)
Figure with time correlation between F11 and BRIKEN
The number of correlations (integrated spectrum minus flat background)
is 73063 very close the number of detected neutrons 73899
The difference 833 agrees well with the expected number of background
neutrons. That is: for every neutron detected in BRIKEN there was an
ion passing through F11 (!?).
There is a funny double structure in the first 20 microsec.
94% of the neutrons are detected within 200microsec
Figure with the spectra of Veto plastics Top (red) and
bottom (blue). There are 7.5 times more counts in T than in B.
One can see in the Top peaks at 3MeV and 12MeV
(corrected from 6 and 25 MeV: wrong calibration!!)
and show signals up to very high energy (GeV)
Figure with the time correlation between Veto Plastics and BRIKEN
Top (red) Bottom (blue). There is a time correlation with Top veto plastic
for 15% of the neutrons in BRIKEN (11440). There are 18 times less
correlations with the Bottom plastic.
WARNING: The correlation was done for signals above "20MeV"
in the V_PL_T spectra i.e. only including the second bump" |
Attachment 1: 161106_0117_62Ni_F11_C6mm_Rates.pdf
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Attachment 2: 161106_0117_62Ni_F11_C6mm_F11.pdf
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Attachment 3: 161106_0117_62Ni_F11_C6mm_CorrBRF11R.pdf
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Attachment 4: 161106_0117_62Ni_F11_C6mm_VPL.pdf
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Attachment 5: 161106_0117_62Ni_F11_C6mm_CorrBRVPL.pdf
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113
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Sat Nov 5 03:36:34 2016 |
Tain et al | Ancillary detectors |
Some info on ancillary detector signals
Plastic veto detectors (Top and Botomm):
The dynode signal of the PMT is passed through an
ORTEC 474 TFA amplifier before going to the DACQ
TFA: Gain=6 x min(~x2), Tint=200ns,Tdif=100ns, NonInvert
DACQ channels: Top: V1A7C1, Bottom: V1A7C2
Photo of the signals of both detectors attached
with 60Co source (with gain changed to 20 x max(~x12.5))
200ns wide 70mV high signal
With this info a rough calibration was established:
for the 2V range an ADC unit is 2000mV/16384=0.122mV
the 70mV (~1MeV) correspond to 574 ADC units which
with the change of gain 6*2/20/12.5=0.048
become 27.6 ADC units. We checked with Gasific
that roughly 1 ADC unit corresponds to 2 EFIR units
thus the calibration is 1/2/27.6=0.018 MeV/unit
NOTE: the calibration in online spectra taken
before noon Sunday 6 was wrong by a factor 2
too large!!!!
Si detector (Top and Bottom halves):
Signal from preamplifier in the low gain mode for the measurement:
we see nothing on the scope with 60Co source. In the high gain mode
we saw the other day a negative 6microsec wide 1mV high
signal with a 60Co.
AIDA plastic veto:
The signal from the PMT is going through a CAEN
shaping amplifier. The signal has a bipolar shape
with a rise time of 500ns a total width of 2microsec
and a height of 100mV (60Co)
F11 ToF plastic (Left and Right):
The signals are processed in the same way that the
plastic veto detector with TFA using the same settings.
Polarity of the signal unknown.
Currently we see no signal seems its not connected.
We found later that the NIM crate where the
TFA were sitting was not on!
We just made a calibration with beam particles
LISE was used to estimate an energy loss of 65 MeV for the ions. |
Attachment 1: VetoBottomPlastic.JPG
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Attachment 2: VetoTopPlastic.JPG
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Attachment 3: AIDAPlasticShaped.JPG
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112
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Sat Nov 5 03:18:13 2016 |
SG BCR RCF NTB | Gamma peaks in the overnight run, related to neutron inelastic scattering |
We looked at the overnight background run (161105_0935_BackgroundOvernight.root), There are gamma-peaks that could be related to neutron inerastic scattering. We identified 565, 596, 608 and 69 keV. They might be related to the effect of neutrons. If this is the correct assignment, this would mean at least some of the neutrons are not thermal when they interact with the germanium.
There was also significant drift in the Ge gain (seen on the pulser) this may effect the shape of these peaks.
Some gain drift was also seen on He preamps during this run. The cause is yet to be determined. It is also yet to be determined if these gain shifts are correlated. |
Attachment 1: 08.png
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Attachment 2: 06.png
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111
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Sat Nov 5 01:26:46 2016 |
Jose,Iris,Alvaro, Alejandro, Krzysztof | Background measurement |
Measurement overnight
Start: around 1:00
Stop: 9:35
File: 161105_0935_BackgroundOvernight.root
The background level after removing the 252Cf source
from the hall dropped to 0.4n/s.
During the night there were neutron rates up to 120 n/s (see figure)
There is a huge spike in the rates which coincides with the time of
LN2 filling. One can see spike in several spectra (not in all)
One can see also a structure superposed
The rate per rings is also shown. The outer rings see
a higher rate.
Also shown is the comparison of He107 one (blue) of the outer ORNL2 tubes
with He084 one (red) of the inner ORLN2. The increase in count rate
is about 30%.
Also shown is the comparison of two external tubes on the top and the bottom:
He107 (blue) and He137 (red), ORNL2 tubes. There is no increase in count rate.
Also shown is the comparison of a tube above the lead shielding He028 (blue)
and behind the lead shielding He048 (red), UPC tubes. There is no difference.
There is also comparison between the rate in the CLOVERS and BRIKEN.
Without beam the rate in the Clovers is around 100 g/s against 0.4 n/s in BRIKEN
At the maximum both rates are similar around 130 c/s.
There is also a plot of the gamma-neutron correlation.
We see that there are neutrons which are detected before
the gammas. A possible explanation several neutrons are produced
one is detected first the second later produces a gamma. |
Attachment 1: 161105_0935_RateBRIKEN.pdf
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Attachment 2: 161105_0935_RateRings.pdf
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Attachment 3: 161105_0935_He107He084.pdf
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Attachment 4: 161105_0935_He107He137.pdf
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Attachment 5: 161105_0935_He048He028.pdf
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Attachment 6: 161105_0935_RateCloversBRIKEN.pdf
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Attachment 7: 161105_0935_CorrBRIKENClovers.pdf
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110
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Sat Nov 5 01:25:24 2016 |
Tain et al | End of Beam Line Setup |
Some photos of the elements in the last part of the beam line
during Takechi run.
After the chamber that includes the F11 plastic detector
there are 2 GSI-MUSIC chambers.
In between the MUSIC chambers there is a sample changer
with 2 Carbon targets of 6mm and 3mm thickness and also
an empty position.
After the 2nd MUSIC there is a plastic detector for testing
(could be removed at any time)
Afterwards there is the degrader mounted on a separate table.
In the same table there is a 10cm thick lead wall
to protect AIDA during Takechi run.
Mounted on the shielding are from the beam side the top and bottom
plastic veto detectors.
On the back side the Si detector is mounted.
The hole in the shielding is covered with
a 2cm thick Al plate to protect AIDA during Takechi run.
Behind AIDA there is a thin plastic detector
to veto the passing through particles. |
Attachment 1: MUSIC-Ctarget-degrader.jpg
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Attachment 2: Ctarget.jpg
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Attachment 3: Degrader-PlasticVeto.jpg
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Attachment 4: VetoPlastic.jpg
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Attachment 5: SiDetector.jpg
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Attachment 6: PlasticBehindAIDA.jpg
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Attachment 7: BRIKEN-AIDA.jpg
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Attachment 8: PlasticBehindMUSIC.jpg
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Attachment 9: LeadBricks.jpg
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109
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Fri Nov 4 13:16:42 2016 |
JLTain,ATolosa,JAgramunt | Neutron Background |
Beam tuning in BigRIPS
At 19:00 access to Exp. Area was closed and the tuning
of BigRips started.
Unfortunately the 252Cf was left on the table close
to the stairs and cannot be removed until 23:00.
We did a background measurement
Start: 19:00
Stop: 22:18
File: 161104_2218_BeamTuning.root
In the attached figure 1 one can see a plot of the rate
(neutrons/10s) in the BRIKEN detector during this time
The rate was at high as 150n/s during this period.
We estimate that the influence of the 252Cf source is about 15n/s
(corresponds to the lowest rates)
Also attached are pictures of the Top and Bottom plastic veto detectors
mounted just above and below the hole in the shielding.
Interestingly the bottom sees less counts at high energy
and this could be related to the 10cm lead wall raised
before the degrader to protect AIDA that covers only partially
the top detector.
Also attached is the neutron spectrum for the different rings superposed.
(ROOT color code) |
Attachment 1: Screenshot_from_2016-11-04_22-26-10.png
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Attachment 2: Screenshot_from_2016-11-04_22-35-46.png
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Attachment 3: Screenshot_from_2016-11-04_22-35-29.png
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Attachment 4: Screenshot_from_2016-11-04_22-43-32.png
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108
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Fri Nov 4 03:37:27 2016 |
Roger Caballero | Energy calibration for Ge clovers |
Energy Calibration: See attached pdf
Detector Slope Offset
V2A7C1 0.00155643 0.0842245
V2A7C2 0.000658962 0.78685
V2A7C3 0.00153391 1.198
V2A7C4 0.00157933 0.483094
V2A7C5 0.000704268 0.31553
V2A7C6 NOT THERE
V2A7C7 0.00066837 0.465225
V2A7C8 0.000695872 0.678058
> Energy calibration for clovers, 152Eu
>
>
>
> The Eu source positioned in the center roughly.
> File name: 161103_1426_152Eu.root |
Attachment 1: 20161104-HpGe-EnergyCal.pdf
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107
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Thu Nov 3 23:28:01 2016 |
A. Tolosa | BRIKEN Bkg + 152Eu |
Measurement over night with a 152Eu source inside
Start: 22:48 (03/11/2016)
Stop: 08:26
File: 161104_0826_152Eu.root
Neutron background rate: 0.82 n/s |
Attachment 1: 161104_0826_152Eu.png
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Attachment 2: 161104_0826_152Eu_CLOVERS.png
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106
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Thu Nov 3 15:09:52 2016 |
A. Tarifeno-Saldivia, C. Domingo-Pardo, J.L. Tain | BRIKEN neutron efficiency |
Geant4 BRIKEN Neutron efficiency calculations as a function of neutron energy and for some spectra: Ga84-vandle, Br88-endf71, Rb94-endf71, Rb95-endf71, I137-endf71, Cf252-MCNPX
Calculations for the current BRIKEN detector configuration:
Hybrid mode, 140 counters, assembled in July16.
Summary of files:
BRIKEN_hybrid140.svg ---> Scheme for the current tube configuration.
BRIKEN_hybrid140_efficiency.xlsx ---> Sheet with results of the calculations.
Efficiency_vs_Energy_HybridConf_140b.svg ---> Plot of the neutron efficiency by Ring (see BRIKEN_hybrid140.svg) and total. |
Attachment 1: BRIKEN_hybrid140.svg
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Attachment 2: Efficiency_vs_Energy_HybridConf_140b.svg
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Attachment 3: BRIKEN_hybrid140_efficiency.xlsx
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105
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Thu Nov 3 14:02:49 2016 |
Nepal, J Ha, PV, Liu J | The degrader system has been set |
We used the laser to align the degrader (see attached photos)
According to the LISE calculation, equivalent effective thickness for 6 mm of Carbon target is 4.5 mm thick Aluminum.
Therefore, we've set the degrader system as follow:
No
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Thickness
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Center Position(maybe a little shift)
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Remove Position(maybe a little shift)
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1
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2.2 mm
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+ Maximum(+ 99676)
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Home (0)
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2
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1.0 mm
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+ Maximum(+ 85042)
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Home (0)
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3
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2.2 mm
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+ Maximum(+ 84962)
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Home (0)
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Control PC IP:10.32.6.153
user: decay
password: d******8
Click Logitec ??QuickCam and SEGEMCS to view the camera
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Attachment 1: IMG_1318.JPG
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Attachment 2: IMG_1317.JPG
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104
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Thu Nov 3 05:46:48 2016 |
Iris, Ale | Background measurement |
Background measurement for threshold determination
Started at 14:45
Stopped: 16:35
Root file: 161103_1635_bck.root |
103
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Thu Nov 3 05:27:48 2016 |
Alvaro, Tain, Gabor, Ale | 152Eu |
Energy calibration for clovers, 152Eu
The Eu source positioned in the center roughly.
File name: 161103_1426_152Eu.root |
Attachment 1: 161103_1426_152Eu.root
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102
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Thu Nov 3 04:46:24 2016 |
Alvaro Tolosa | 252Cf |
Check of BRIKEN calibration and thresholds
Source more or less at the center
Online File: 161103_1319_252Cf.root |
Attachment 1: 161103_1319_252Cf.root
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101
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Thu Nov 3 04:40:02 2016 |
All | START |
Start of commissioning preparation
Working directory:
/data/1611Commissioning/161031Preparation/
DACQ configuration file:
161103Conf_BrikenFull.xlsx |
Attachment 1: 161103Conf_BrikenFull.xlsx
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100
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Wed Nov 2 02:26:22 2016 |
Roger Caballero | Efficiency callibration calculator (Excel file) |
Attached the updated excel file. In the first sheet there is the calculator to calculate the efficiency from an given energy.
The Jackel function used is:
Double_t fun=TMath::Exp((par[0]+par[1]*TMath::Log(x[0])+par[2]*TMath::Log(x[0])*TMath::Log(x[0]))*2/TMath::Pi()*
(TMath::ATan(TMath::Exp(par[3]+par[4]*TMath::Log(x[0])+par[5]*TMath::Log(x[0])*TMath::Log(x[0]))))-25.);
> Efficiency calibration
>
> File "cloversEff.ods" and "cloversEff.xls" contains the experimental efficiency from different measurements
> during July and October
> (G7 broke before Eu-152 measurement). We can assume the efficiency didn't change from July measurements to
> October measurements. |
Attachment 1: cloversEff.xls
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99
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Wed Nov 2 01:19:46 2016 |
Roger Caballero | Eff callibration parameters for D4-Clover |
Efficiency calibration for the D4 clover (data acquired in October).
The attached plots show the parameters for the Jackel function (E[i]=Energy) using the points of 152Eu, 60Co and 137Cs sources.
Roger
> Efficiency calibration
>
> File "cloversEff.ods" and "cloversEff.xls" contains the experimental efficiency from different measurements
> during July and October
> (G7 broke before Eu-152 measurement). We can assume the efficiency didn't change from July measurements to
> October measurements. |
Attachment 1: D4-Black.pdf
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Attachment 2: D4-Red.pdf
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Attachment 3: D4-Green.pdf
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Attachment 4: D4-Blue.pdf
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97
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Tue Nov 1 13:00:55 2016 |
Roger Caballero | Eff callibration parameters for G7-Clover |
Efficiency calibration for the G7 clover (data acquired in July).
The attached plots show the parameters for the Jackel function (E[i]=Energy) using the points of a 152Eu source.
Roger
> Efficiency calibration
>
> File "cloversEff.ods" and "cloversEff.xls" contains the experimental efficiency from different measurements
> during July and October
> (G7 broke before Eu-152 measurement). We can assume the efficiency didn't change from July measurements to
> October measurements. |
Attachment 1: G7-Blue.pdf
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Attachment 2: G7-Green.pdf
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Attachment 3: G7-Red.pdf
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Attachment 4: G7-Black.pdf
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96
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Tue Nov 1 09:27:02 2016 |
Alvaro Tolosa | CLOVER |
Efficiency calibration
File "cloversEff.ods" and "cloversEff.xls" contains the experimental efficiency from different measurements
during July and October
(G7 broke before Eu-152 measurement). We can assume the efficiency didn't change from July measurements to
October measurements. |
Attachment 1: cloversEff.xls
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Attachment 2: cloversEff.ods
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95
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Mon Oct 31 23:56:37 2016 |
J. Agramunt | First AIDA BRIKEN correlation plot |
From the 252Cf data. |
Attachment 1: FirstAIDA_BRIKENPlot.pdf
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94
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Tue Oct 18 09:41:43 2016 |
Alvaro Tolosa | 2016 - July, Logbook |
Paper logbook for July-2016
For correct visualization,
please download it. |
Attachment 1: 16Jul_logbook.pdf
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93
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Tue Oct 18 09:36:07 2016 |
Alvaro Tolosa | 2016-Oct, Logbook |
Paper logbook for October-2016
For correct visualization,
please download it. |
Attachment 1: 16Oct_logbook.pdf
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92
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Mon Oct 17 05:21:46 2016 |
Phong, Liu J J | dE detector position and output signal from preamplifier |
dE detector is mounted onto the back side of the shielding (attached photo: dE_position.JPG)
The detector consists of 26 strips. In this setup, the detector is devided into 2 parts corresponding to 2 readout channels. Each part consists of 13 strips joint together.
Output signal from a high gain channel of preamplifier with 137Cs source is shown in attachment 137CsTest_ac.JPG.;
The white noise is about 2 mV for high gain mode.
We will switch to low gain mode during the experiment.
* note:there is a 200 mV offset due to the characteristic of the preamplifier (see attachment dc.JPG) |
Attachment 1: 137CsTest_ac.JPG
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Attachment 2: dE_position.JPG
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Attachment 3: dc.JPG
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91
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Sun Oct 16 13:30:43 2016 |
All | END |
... and sashimi (see photo)
The detectors (BRIKEN tubes, CLOVER, VETO detectors, AIDA)
are mounted, tested and ready for November commissioning,
except beam detectors a Plastic TOF and a Si detector which
will be attached to the PE shielding.
DACQs (BRIKEN, AIDA) are running. The synchronization monitoring
program which was working in June, for some reason is not functioning
properly now and is being worked on (desirable but not required).
The data merger and near-line analysis programs are being worked on. |
Attachment 1: Sashimi.jpg
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90
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Sun Oct 16 12:58:34 2016 |
All | BRIKEN |
Installation of BRIKEN PE shielding for beam
related neutrons
The missing metallic pieces needed to mount
the forward PE shielding finally arrive and
we mount it with help of the crane.
The shielding (4 PE slabs + 1Cd-PE slab) has attached
the support for VETO detectors on the beam side
and for and additional ancillary detector
a large Si detector on the BRIKEN side.
See attached photos.
The distance between shielding and BRIKEN is 40 cm. |
Attachment 1: Shielding-BRIKEN-AIDA.jpg
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Attachment 2: Shielding-BRIKEN.jpg
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Attachment 3: ShieldingPlates.jpg
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89
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Fri Oct 14 14:06:38 2016 |
All | First measurement of BRIKEN and AIDA |
Friday, October 14, 2016 21:50
AIDA and BRIKEN-CLOVER run with a common clock.
After installing the shielding and checking electronics
(See next entry)
252Cf source 7.5cm from the center.
AIDA nose aligned with the edge of the clovers hole.
start: 21:50 run number: BRIKEN:15 AIDA:0
stop : 22:18 run number: BRIKEN:16 AIDA:9
BRIKEN dlt file:252CfWithAida75mmcenter_15 to _16
AIDA file: aidas1:/TapeDate/Sept2016/R41_0 to _9
Online analyzed data around 30%
Online spec: 252CfWithAida75mmcenter_15_16.root
Configuration file attached. |
Attachment 1: 161014Conf_BrikenFull.xlsx
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88
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Fri Oct 14 13:32:52 2016 |
NT BREWER, S Go, JM Allmond | Ge preamp power loss and solution. |
As previously recorded (81), on Thur Oct 13th, A NIM crate failure caused preamp power loss to the HPGe's. While D4 recovered with nominally the same resolution as before. G7 would not recieve power to the preamps without an alarm from the NIM crate.
It was determined that there was a short along the lines of +12V and Ground , -12V and Ground, and between +-12V.
After removing the Red preamp ribbon cable, the remaining channels (K,G,B) were able to be powered on and found to have a nice resolution of near ~2.3 keV for 661 (137Cs).
During the course of testing, the preamp power distribution box (supplied from ORNL) was seen to have a fault in the +12V light and supply. This was seen by placing this supply in a new NIM bin and seeing that it would also not properly supply preamp power to clover D4 (which had recovered fully).
The consistency in this fault is seen as cause to be suspicious of this preamp power supply. It has been replaced by putting two ORTEC TSA's into a seperate NIM bin and using the standard power supply for D4 and G7.
There was no appreciable effect on noise in any other detector.
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87
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Fri Oct 14 04:42:40 2016 |
JL Tain et al | Electronics |
Change of main power line for MPOD and CLOVER preamp
Because the incident yesterday with the NIM crate,
we try to separate the CLOVER from the rest of
the equipment.
So we put the MPOD, which powers the CLOVER but also
the 3He tubes and the VETO detectors, and the preamp
power supply in a different line.
We check if this has an impact on the noise in either
CLOVER or 3He tubes.
We measure with the 137Cs-60Co source:
File: 161014_1241_137Cs60Co.root
After inspecting the spectra we conclude that the impact
is not appreciable.
See figures
662keV resolution:
D4Black: 3.16keV
D4Red: 2.49keV
D4Green: 3.57keV
D4Blue: 3.40keV |
Attachment 1: D4All-CsCo-zoom-newlineCL.pdf
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Attachment 2: BRIKEN-newlineCL.pdf
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86
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Fri Oct 14 04:12:50 2016 |
JL Tain et al | CONF |
New configuration file:
161014Conf_BrikenFull.xlsx |
85
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Thu Oct 13 23:42:27 2016 |
JL Tain et al | Background |
Background measurement overnight
Start: 01:17
Stop: 10:35
File: 161014_1035_bck.root
See figure |
Attachment 1: Bckg-161014.pdf
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84
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Thu Oct 13 23:41:25 2016 |
JL Tain et al | 252Cf |
New BRIKEN energy calibration
We check the 3He tubes energy calibration with 252Cf source
We Found that only one tube He006 was slightly shifted and correct it.
Check measurement:
File: 161014_0113_252Cf.root
See figure |
Attachment 1: 252Cf-161014.pdf
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83
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Thu Oct 13 23:39:58 2016 |
JL Tain et al | VETO Det |
Energy calibration of plastic and NaI detectors
137Cs source placed in the center of the arrangement:
two plastics on top of each other the four NaI
on the sides. See photo.
First measurement:
File: 161014_0015_137Cs_VetoDetCal.root
after calibration check measurement:
File: 161014_0038_137Cs_VetoDet.root
60Co source: 161014_0047_60Co_VetoDet.root
See figures
ADC ranges at the moment:
Plast: 20 MeV
NaI: 20 MeV |
Attachment 1: Plast-Cs.pdf
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Attachment 2: NaI-Cs.pdf
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Attachment 3: Plast-Co.pdf
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Attachment 4: NaI-Co.pdf
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Attachment 5: VETO-testarrangement.jpg
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82
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Thu Oct 13 23:38:26 2016 |
JL Tain et al | CLOVER |
Energy and efficiency calibration
We make calibrations for the remaining D4 CLOVER detector
(No pulser: D4 preamp does not see the pulser input, a single TEST input)
Sources on the cardboard holder, place at the center of BRIKEN
137Cs (Ref:CD393) together with 60Co (Ref:CD395):
File: 161013_2331_137Cs60Co.root
152Eu (Ref:272/09-7011):
File: 161013_2350_152Eu.root
The threshold in Black,Green and Blue is cutting Ba X-rays.
Activity of the sources:
>> 60Co (Ref:CD395): 338.4 kBq (+-3%) measured on 01.07.1990
>> 137Cs (Ref:CD393): 347.9 kBq (+-3%) measured on 01.07.1990
>> 152Eu (Ref:272/09-7011): 10.62 kBq (+-1,9%) measured on 16.03.2010
See figures. |
Attachment 1: D4All-CsCo.pdf
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Attachment 2: D4All-CsCo-zoom.pdf
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Attachment 3: D4Sum-152Eu.pdf
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81
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Thu Oct 13 12:58:31 2016 |
JL Tain et al | INCIDENT |
NIM Crate Failure. Lost of CLOVER G7
One of the 2 NIM crates, the one containing the power for CLOVER
preamps went kaputt.
As a consequence the preamp of CLOVER detector G7 was damaged:
G7 was removed |
80
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Thu Oct 13 04:36:58 2016 |
JL Tain et al | CLOVER |
CLOVER energy calibration
Short run with 137Cs and 60Co sources at BRIKEN detector center
to make a new energy calibration
Root file: 161013_1240_137Cs60Co.root
We conected the test input to the pulser, and a new calibration was needed
Root file: 161013_1518_137Cs60Co.root |
Attachment 1: 161013_1518_137Cs60Co.root
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79
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Wed Oct 12 11:30:53 2016 |
Ariel Tarifeno, Alvaro Toloza, JL Tain, J. Agramunt, et al | BRIKEN Z scan |
Scanning of the BRIKEN detector with the 252Cf source
along the longitudinal axis (Z axis)
Measurements from Z: -42.5cm to 42.5cm with steps of 2.5cm. |
78
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Wed Oct 12 05:06:57 2016 |
JL Tain et al | Noise |
Gamma source close to ORNL2 tube
In order to investigate the origin of the background
component in ORNL tubes extending up to 200keV
we place a strong 137Cs source (D393) in the hole
of He136 close to the tube.
Control measurement (no source): 161012_1200_bck_control.root
With source: 161012_1229_137CsHe136.root
We observe that the induced signals are in the same energy region
as the 3rd noise component. The increase of the rate of signals
with the source is a factor 60.
See figures.
This hints to the origin of this component as due to an increased sensitivity
to gamma-rays (more material?) or internal radioactivity (gamma,beta)
of ORNL tubes. |
Attachment 1: He136-nosource.pdf
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Attachment 2: He136-137Cs.pdf
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77
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Wed Oct 12 03:47:14 2016 |
JL Tain et al | Background |
Background measurement over night with CLOVER and VETO detectors
ADC #7 added to crate 1 for veto detectors: V1A7
VETO detectors HV off!
Start: 23:45
Stop: 10:56
File: 161012_1056_bck_noise.root
We see a very strong noise in the BRIKEN spectrum!!!
After some work we find that this was a problem
with configuration file: when editing the file
we put the calibration sheet at the beginning this
provoked a mixing of CLOVER and 3He spectra. |
76
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Tue Oct 11 17:11:28 2016 |
A. Tarifeno-Saldivia et al... | ROOT macro |
ROOT macro for calculation of neutron rates in the BRIKEN detector
Here a ROOT macro to calculate neutron rates from onlines root files generated DAQ configuration
160718Conf_BrikenFull_cal5.xlsx (and the later ones).
Setup parameters are indicated at the begining of the macro. An output data file is generated with the rates by counter, ring and ADC. If the input root file is "file.root", the
output data file is "file.root_data".
Further questions by email to: atarisal@gmail.com
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Attachment 1: BRIKEN_rates_v3.cc
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//ROOT macro for calculation of neutron rates in the BRIKEN detector
// A. Tarifeno-Saldivia && A. Tolosa, Date: 12Oct16, update 12Oct16
TH1F* h_sum = NULL;
void BRIKEN_rates_v3(){
gStyle->SetOptStat("nei");
//**************** SETUP ****************
int Ndet_i=1;
int Ndet_f=140;
Double_t deltaPulser=30.0;
Double_t PulserLowLimit=1350.0;
Double_t Emin = 160.0; // in keV
Double_t Emax = 900.0; // in keV
Double_t PeakAmplitude_threshold=0.005; // 0.005 should work.
// Higher values than 0.08 may affect finding pulser position
//*****************************************
TString input;//="0cm_2.root";
cout<<"Existing root files in current directory: \n";
gSystem->Exec("ls *.root");
cout<<"Input root file: \n";
cin >> input;
TFile * file = TFile::Open(input);
ofstream outFile(input + "_data");
TH1F * inter = (TH1F*) file->Get("He001");
h_sum = (TH1F*) inter->Clone();
h_sum -> Reset();
h_sum->SetName("Sum histogram");
h_sum->SetTitle("BRIKEN full histogram: " + input);
TString histName;
TCanvas *C1= new TCanvas("C1", "C1", 1);
C1->cd();
double Counter_nRates[141];
for(int i=0 ; i < 141 ; i++){Counter_nRates[i]=0.0;}
Double_t TotalnRate=0.0;
outFile<<"# File:\t"<<input<<endl;
outFile<<"# Histograms size:\t"<<h_sum->GetSize()<<endl;
outFile<<"# Emin:\t"<<Emin<<" keV\tEmax:\t"<<Emax<<" keV\n";
outFile<<"# deltaPulser:\t"<<deltaPulser<<" keV\tPulserLowLimit:\t"<<PulserLowLimit<<" keV\n";
outFile<<"#####################################################################################################\n";
outFile<<"# Detector\tnRate\tNeutronCounts\tPulserCounts\tpulserPos\tPeakBINo\tPeakBINf\n";
outFile<<"#\t\t(counts\t(counts)\t (counts)\t(keV)\t \t(bin)\t \t(bin)\t\n";
outFile<<"#\t\t/pulser)\n";
outFile<<"#####################################################################################################\n";
for(int i=Ndet_i; i<=Ndet_f ; i++){
if(i>0 && i<10) histName= Form("He00%d", i);
if(i>=10 && i<100) histName= Form("He0%d", i);
if(i>=100 && i<=140) histName= Form("He%d", i);
TH1F* hi =(TH1F*)file -> Get(histName);
// Find peak for pulser
TSpectrum *s = new TSpectrum(100);
Int_t nfound = s->Search(hi,10,"",PeakAmplitude_threshold);
TList *functions = hi->GetListOfFunctions();
TPolyMarker *pm = (TPolyMarker*)functions->FindObject("TPolyMarker");
Double_t* pmarrayX=pm->GetX() ; // Find polymarkers position
Double_t pulserPos, PulserCounts, NeutronCounts, nRate;
bool found=false;
int peakCounter=0;
int BinEmin= hi->GetXaxis()->FindBin(Emin);
int BinEmax= hi->GetXaxis()->FindBin(Emax);
for (int j = 0; j < nfound; j++) {
pulserPos=pmarrayX[j];
if(pulserPos>=PulserLowLimit){
peakCounter++;
found=true;
TF1 *f1 = new TF1("f1","gaus",-.5,.5);
f1->SetParameters(1000.0, pulserPos, deltaPulser);
hi -> Fit("f1", "Q", "",pulserPos-deltaPulser,pulserPos+deltaPulser);
Double_t mean = f1->GetParameter(1);
Double_t sd = f1->GetParameter(2);
Double_t Peak_o=mean-3.5*sd;
Double_t Peak_f=mean+3.5*sd;
int PeakBINo= hi->GetXaxis()->FindBin(Peak_o);
int PeakBINf= hi->GetXaxis()->FindBin(Peak_f);
PulserCounts = hi->Integral(PeakBINo,PeakBINf);
NeutronCounts = hi->Integral(BinEmin,BinEmax);
nRate=NeutronCounts/PulserCounts;
Counter_nRates[i]=nRate;
//TotalnRate+=nRate;
outFile<<histName<<"\t"<<nRate<<"\t"<<NeutronCounts<<"\t"<<PulserCounts<<"\t";
outFile<<pulserPos<<"\t"<<Peak_o<<"\t"<<Peak_f<<"\t"<<endl;
// cout<<histName<<"\t"<<nRate<<"\t"<<NeutronCounts<<"\t"<<PulserCounts<<"\t";
// cout<<pulserPos<<"\t"<<PeakBINo<<"\t"<<PeakBINf<<"\t"<<hi->GetSize()<<endl;
}
if(j==nfound-1 && found==false){
outFile<<histName<<"\t -------> ERROR FINDING THE PULSER, CHECK PeakAmplitude_threshold !!!!!\n";
cout<<histName<<"\t -------> ERROR FINDING THE PULSER, CHECK PeakAmplitude_threshold !!!!!\n";
}
if(j==nfound-1 && found==true && peakCounter>1){
outFile<<histName<<"\t -------> MORE THAN ONE PULSER POSITION, CHECK PeakAmplitude_threshold !!!!!\n";
cout<<histName<<"\t -------> MORE THAN ONE PULSER POSITION, CHECK PeakAmplitude_threshold !!!!!\n";
}
}
h_sum -> Add(hi);
}
outFile<<"\n#######################################################################\n";
outFile<<"# NEUTRON RATES (counts/pulser)\n";
outFile<<"#######################################################################\n";
//**************** Rates Calculation:
// ADC arrays
int V1A[6][16]={{1,2,3,4,5,6,7,8,9,10,11,12,21,22,23,24},
{13,14,15,16,17,18,19,20,31,32,33,34,35,36,37,38},
{25,26,27,28,29,30,43,44,45,46,47,48,49,50,51,52},
{39,40,41,42,53,54,55,56,57,58,59,60,61,62,63,64},
{65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80},
{81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,0}};
int V2A[6][8]= {{96,97,98,99,100,101,102,103},
{104,105,106,107,108,109,110,0},
{111,112,113,114,115,116,117,118},
{119,120,121,122,123,124,125,0},
{126,127,128,129,130,131,132,133},
{134,135,136,137,138,139,140,0}};
int Ri[7][28]={{1,2,3,7,8,9,21,13,14,15,19,20,26,27,28,29,30,46,47,48,49,50,0,0,0,0,0,0},
{4,5,10,11,22,23,16,17,33,34,35,36,53,54,55,56,0,0,0,0,0,0,0,0,0,0,0,0},
{6,12,24,18,31,32,37,38,25,43,44,45,51,52,39,40,41,42,57,58,59,60,61,62,63,64,0,0},
{66,67,74,75,81,82,83,84,85,111,112,113,114,115,0,0,0,0,0,0,0,0,0,0,0,0,0,0},
{65,68,73,76,86,87,88,89,90,91,116,117,118,119,120,121,0,0,0,0,0,0,0,0,0,0,0,0},
{92,93,94,95,96,97,98,99,100,122,123,124,125,126,127,128,129,130,0,0,0,0,0,0,0,0,0,0},
{69,70,71,72,77,78,79,80,101,102,103,104,105,106,107,108,109,110,131,132,133,134,135,136,137,138,139,140}};
//total
for(int i=0 ; i < 141 ; i++){TotalnRate+=Counter_nRates[i];}
cout<<"#########################################\n";
cout<<"# Total neutron rate (counts/pulser):\t"<<TotalnRate<<endl;
cout<<"#########################################\n";
cout<<" RATE BY RING:"<<endl;
cout<<"---------------"<<endl;
outFile<<"Total neutron rate:\t"<<TotalnRate<<endl;
outFile<<"#########################################\n";
outFile<<" BY RING:"<<endl;
outFile<<"#########################################\n";
for(int i=0 ; i < 7 ; i++){
double ringRATE=0.0;
for(int j=0 ; j < 28 ; j++){
ringRATE+=Counter_nRates[Ri[i][j]];
}
cout<<"R"<<i+1<<"\t"<<ringRATE<<endl;
outFile<<"R"<<i+1<<"\t"<<ringRATE<<endl;
}
outFile<<"#########################################\n";
outFile<<" BY ADC:"<<endl;
outFile<<"#########################################\n";
cout<<"#########################################\n";
cout<<" RATE BY ADC:"<<endl;
cout<<"---------------"<<endl;
//By ADC
//VME1
for(int i=0 ; i < 6 ; i++){
double vmeRATE=0.0;
for(int j=0 ; j < 16 ; j++){
vmeRATE+=Counter_nRates[V1A[i][j]];
}
cout<<"V1A"<<i+1<<"\t"<<vmeRATE<<endl;
outFile<<"V1A"<<i+1<<"\t"<<vmeRATE<<endl;
}
//VME2
for(int i=0 ; i < 6 ; i++){
double vmeRATE=0.0;
for(int j=0 ; j < 8 ; j++){
vmeRATE+=Counter_nRates[V2A[i][j]];
}
cout<<"V2A"<<i+1<<"\t"<<vmeRATE<<endl;
outFile<<"V1A"<<i+1<<"\t"<<vmeRATE<<endl;
}
h_sum -> Draw();
gPad->SetLogy();
outFile.close();
//gApplication->Terminate();
}
|
75
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Tue Oct 11 15:58:01 2016 |
JL Tain et al | VETO Det |
Check of Plastic and NaI veto detectors and DACQ settings
Plastic: 10x200x450mm**3, PMT: H1161, HV: -1200V, Anode2
Very small and short signal: width: 20ns, rise: 10ns, amplitude up to 10mV
We decided to put an amplifier to have more flexibility
Amp: Ortec 474 TFA, G: 10xmax, INT=200ns, DIF: 100ns
Signal: width: 200ns, height: 100mV
DACQ Trigger & EFIR: P=2, G:2
NaI: 2"x4"x16", PMT: ?, VD: 1410 (ORNL), HV: +800V
Signal: width: 400ns height: 15mV
DACQ trigger and EFIR: P=20, G=20
File: 161011_2330_PlasticNaI_137Cs.root
File: 161011_2335_PlasticNaI_60Co.root
Photo of the arrangement.
137Cs spectrum of both detectors. |
Attachment 1: IMG_20161012_124010.jpg
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Attachment 2: Plastic-137Cs.pdf
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Attachment 3: NaI-137Cs.pdf
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74
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Tue Oct 11 15:47:45 2016 |
N Brewer, S Go et al | CLOVER |
Both COVER detectors are installed in place.
See photos.
Detector D4: left of the beam
Crystal distribution:
BLUE-BLACK
RED -GREEN
Detector G7: right of the beam
Crystal distribution:
BLUE-BLACK
RED -GREEN
Cables connected. Some work on noise minimization.
Resolution improved for D4-Black which was poor
on July. Otherwise similar behaviour.
See spectra with 137Cs and 60Co sources ta the center.
File:161011_1805_CLOVER_CsCo.root
We are using the calibration from July which
works surprisingly well for all except G7Red
(explains double peak in spectrum)
More checks to be done. |
Attachment 1: IMG_20161011_182318.jpg
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Attachment 2: IMG_20161011_182258.jpg
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Attachment 3: D4-1st.pdf
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Attachment 4: G7-1st.pdf
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73
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Sun Oct 9 18:19:01 2016 |
JL Tain et al | Noise |
Optimization of ADC thresholds
In order to try to reduce the grass-like background
we make a finer adjustment of individual ADC thresholds.
We make first a control measurement putting the 252Cf source
in the center of the detector (AIDA removed)
Start: -
Stop: 23:55
File: 161009_2355_252Cf_control.root
We then make an adjustment of thresholds one ADC at a time.
We adjusted the threshold so that the very low amplitude noise height
in the spectrum is only a small fraction of the pulser.
New configuration file: 160718Conf_BrikenFull_test02_thr.xlsx
A verification measurement with 252Cf
Start: 01:55
Stop: 02:09
File: 161010_0209_252Cf_newthr.root
And the leave a background measurement overnight:
Start: 02:12
Stop: 07:12
File: 161010_0712_bck_newthr.root
We compare the grass-noise rates now with the rates before threshold adjustment
For that we integrate the BRIKEN spectrum between 900keV and 1.5MeV
The rate before was 0.085 counts per second per MeV
The rate now is 0.039 counts per second per MeV
So the improvement was only a factor 2.
One can try to set the thresholds higher however with this rate the probability
of having a noise signal in a 0.5ms window after a beta signal will be about 1E-5.
The plots below show the situation before and after. |
Attachment 1: 161007_1045_bck_lin.pdf
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Attachment 2: 161010_0712_bck_newthr.pdf
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72
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Sun Oct 9 15:49:41 2016 |
JL Tain et al | Power shutdown |
Due to maintenance operations of the Wako electrical
company there is a risk of power shutdowns on Saturday,
Sunday and Monday from about 8 am to 8 pm.
So we have to stop working on the hardware during
this time |
71
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Sun Oct 9 04:20:47 2016 |
JL Tain et al | Noise |
We check for the appearance of spurious signals in the preamplifiers.
We set all HV to zero and run a measurement for several hours.
Start: October 7, 20:00
Stop: October 8, 06:42
File: 161008_0642_noHV.root
De inspection of the different channels do not reveal any
particular problem.
See figure for channels grouped in rings |
Attachment 1: noHV.pdf
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Attachment 2: 161008_0642_noHV.pdf
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70
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Sat Oct 8 01:18:51 2016 |
JL Tain et al | DACQ |
We increased the pretrigger delay for ADC5 from 350 to 400 |
68
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Fri Oct 7 10:42:52 2016 |
JL Tain et al | Noise |
We investigate the effect on the noise in ORNL tubes of using a differential PA.
We connect the tubes in current PA10 (126-140) to one of the new diff PA
and connect the output to converter card #4 which is connected to ADC3 (and ADC4).
First a short run with 252Cf for setting the right parameters and the calibration
file: 161007_1743_252Cf_ORNL_diffPreamp.root
Then we make a background run
file: 161007_1743_bck_ORNL_diffPreamp.root
As can be seen in the figure the effect of the differential preamp is to
compress the noise down to 100keV, becoming more similar to
the situation of the RIKEN tubes.
Thus it will be beneficial to use Diff PA. However as we can only setup one
because we have only one spare Diff-Unip converter card, we decided not to
use it as the impact will be very low and implies a lot of changes.
However one must remember that since we are always going to require coincidence
with betas during the measurement this noise should have no effet. |
Attachment 1: ORNL-DiffPreamp.pdf
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67
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Fri Oct 7 08:35:15 2016 |
JL Tain et al | Noise |
Low amplitude noise component.
The figure shows the composition of the low amplitude noise
which depends on the tube and type of preamplifier used.
Bkack: He020 (RIKEN-Diff)
Red: He044 (UPC-Diff)
Green: He057 (UPC-Unip)
Blue: He068 (ORNL1-Unip)
Pink: He132 (ORNL2-Unip)
(all the tubes of the same type and preamp type behave alike)
We can see up to three different structures.
The noise in the ORNL tubes extends to higher energies (200keV)
and are the cause for the overlap of noise with neutron signals,
but other wise the shape is similar to RIKEN tubes.
The noise for UPC above 50kev is quite small.
One can also see a small difference between differential and unipolar PA
in the case of UPC tubes (red and green) |
Attachment 1: noiseDifferentTubes2.pdf
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66
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Fri Oct 7 08:09:47 2016 |
JLTain et al | Background |
Background measurement overnight
Start: Oct-6 2242 Stop: Oct-7 10:45
file: 161007_1045_bck.root
See attached figure.
We see that low amplitude noise overlaps with the neutron spectrum.
We also see the grass-like background which extends all the way
up to the ADC range. |
Attachment 1: Bckg-1st.pdf
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Attachment 2: 161007_1045_bck.pdf
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65
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Thu Oct 6 14:50:30 2016 |
JL Tain, A Tolosa, A Tarifeno,... | 252Cf |
First measurement with 252Cf source to check the calibration.
AIDA was in place so the source was at the right height
but displaced about 10cm from the center.
We use the last configuation file used in July:
160718Conf_BrikenFull_cal5.xlsx
tmeas=25min
file: 161006_2235_252Cf.root
The noise is rather small.
The calibration of July is nearly OK! |
Attachment 1: 252Cf-1st.pdf
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Attachment 2: 161006_2235_252Cf.pdf
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64
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Thu Oct 6 14:43:47 2016 |
JL Tain, A Tarifeno, A Tolosa, J Agramunt, N Brewer, S Go, ... | Electronics |
We mount back all preamplifiers
Initially we used all the PA coming from US, the repaired and the new ones.
There was an issue with the new ones (strong noise and cross talk)
until we realized that the new ones were of differential type
instead of unipolar. We decided to mount all unipolar so we use
the repaired ones plus the ones which were left here and
had some minor problems with discharges.
We decided to change slightly the gain of the pulser signals
because for PA6 to PA10 the amplitude after the preamp was 2.2-2.4V
so it was saturating the ADC.
So we decreased Pulser 1 (RIKEN, ORNL1, ORNL2, CLOVER)
from 690mV to 540mV (NEG) on the scope (50ohm)
and increased Pulser 2 (UPC) from 90mV to 100mV |
63
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Thu Oct 6 02:03:32 2016 |
JL Tain | START |
We started the assembly of BRIKEN and AIDA detectors in their final position
on Tuesday October 4:
Gabor Kiss, Phong Vi, Keishi Matsui, Shunji Nishimura, Shigeru Kubono, PA,
Chris Griffin, Tom Davinson, Nathan Brewster, Shintaro Go, Daniel Stracener,
Ariel Tarifeno, Jorge Agramunt, Alvaro Tolosa, Jose L Tain
Tubes were removed from BRIKEN. PE matrix lifted with crane.
Table rotated and placed in the final position (front wheels
between forward EURICA rails) by hand. Table leveled (height, angle)
with the help of laser. PE matrix placed back.
AIDA rotated and adjusted to BRIKEN by hand.
See photos |
Attachment 1: BRIKEN-AIDA.jpg
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Attachment 2: BRIKENfront.jpg
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Attachment 3: AIDAback.jpg
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Attachment 4: AIDAintoBRIKEN.jpg
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Attachment 5: AIDAnosefront.jpg
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Attachment 6: AIDA-CLOVERhole.jpg
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62
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Thu Aug 18 23:32:59 2016 |
NT Brewer | New preamps arrived at Oak Ridge and tested working. |
Collaborators,
Attached is a phone photo of example signals from the new preamps with 3 3He tubes connected to a scope. Scope channels 1,2,3 (color y,c,m respectively) are preamp channels 1,2,3 while 4 (green) is open. Trigger is on channel 3, at 500mV/div and other channels are at 500,200,and 20 mV/Div for channels 2,1,4 respectively. Time scale, though glared out should be 10us per div ( although we saw longer rise times as well).
Signals were all good for all channels. Coincident with real signals were other negative signals ~15x (750mV/50mV magenta/green) smaller and with a different shape. No positive signals were observed in any channel.
This picture is representative of the signals of 2 new preamps as well as the functional spare already at UT.
Additionally, the two preamps sent for repair have been received.
NTB, KPR
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Attachment 1: IMG_20160818_145801.jpg
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Attachment 2: IMG_20160803_160430.jpg
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Draft
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Thu Aug 18 22:39:35 2016 |
NT Brewer | New preamps arrived at Oak Ridge and tested working. |
Collaborators,
Attached is a phone photo of example signals from the new preamps with 3 3He tubes connected to a scope. Scope channels 1,2,3 (color y,c,m respectively) are preamp channels 1,2,3 while 4 (green) is open. Trigger is on channel 3, at 500mV/div and other channels are at 500,200,and 20 mV/Div for channels 2,1,4 respectively. Time scale, though glared out should be 10us per div ( although we saw longer rise times as well).
Signals were all good for all channels. Coincident with real signals were other negative signals ~15x (750mV/50mV magenta/green) smaller and with a different shape. No positive signals were observed in any channel.
This picture is representative of the
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Attachment 1: IMG_20160818_145801.jpg
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60
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Fri Jul 29 09:52:28 2016 |
Keishi Matsui | accuracy of Cf-252's intensity in RIKEN |
According to the reply from Japan Radioisotope Association, the accuracy of the Cf-252's intensity is +0%/-15%.
( "+0%" is important, because 3.7 MBq is a standard limit for radio-active sources in Japan.) |
Attachment 1: IMG_9350.JPG
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59
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Fri Jul 22 12:50:29 2016 |
J.L. Tain | END |
20/JUL/2016 20:00
End of the test measurements |
58
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Wed Jul 20 17:21:59 2016 |
J. Agramunt, A. Tolosa | DACQ |
DACQ configuration parameters
The last configuration file used was: 160718Conf_BrikenFull_cal5.xlsx
Most relevant configuration parameters:
3He tubes:
For all channels:
Input: InputRange: 2V, Impedance: 50Ohm
Tigger: Fast filter IntTime: 40, FlatTop: 20
V1A1C1-C16: (RIKEN: PA1,PA2)
Input: Offset: 50000, Polarity: + (POS)
Trigger: GateLength: 800, PreTrigger: 250, Threshold: 2000
Slow Filter: IntTime: 250, FlatTop: 50, Tau: 25000
V1A2C1-C8: (RIKEN: PA2)
Input: Offset: 50000, Polarity: + (POS)
Trigger: GateLength: 800, PreTrigger: 250, Threshold: 2000
Slow Filter: IntTime: 250, FlatTop: 50, Tau: 25000
V1A2C9-C16: (UPC: PA3)
Input: Offset: 50000, Polarity: + (POS)
Trigger: GateLength: 800, PreTrigger: 250, Threshold: 10000
Slow Filter: IntTime: 175, FlatTop: 50, Tau: 25000
V1A3C1-C16: (UPC: PA3,PA4)
Input: Offset: 50000, Polarity: + (POS)
Trigger: GateLength: 800, PreTrigger: 250, Threshold: 10000
Slow Filter: IntTime: 175, FlatTop: 50, Tau: 25000
V1A4C1-C4: (UPC: PA4)
Input: Offset: 50000, Polarity: + (POS)
Trigger: GateLength: 800, PreTrigger: 250, Threshold: 8000
Slow Filter: IntTime: 175, FlatTop: 50, Tau: 25000
V1A4C5-C16: (UPC: PA5)
Input: Offset: 15000, Polarity: - (NEG)
Trigger: GateLength: 1000, PreTrigger: 250, Threshold: 15000
Slow Filter: IntTime: 250, FlatTop: 100, Tau: 25000
V1A5C1-C16: (ORNL1: PA6)
Input: Offset: 15000, Polarity: - (NEG)
Trigger: GateLength: 1000, PreTrigger: 250, Threshold: 3000
Slow Filter: IntTime: 250, FlatTop: 100, Tau: 25000
V1A6C1-C16: (ORNL2: PA7)
Input: Offset: 15000, Polarity: - (NEG)
Trigger: GateLength: 1200, PreTrigger: 350, Threshold: 3000
Slow Filter: IntTime: 350, FlatTop: 100, Tau: 25000
V2A1C1-C8: (ORNL2: PA8) V2A2C1-C8: (ORNL2: PA8)
V2A3C1-C8: (ORNL2: PA9) V2A4C1-C8: (ORNL2: PA9)
V2A5C1-C8: (ORNL2: PA10) V2A6C1-C8: (ORNL2: PA10)
Input: Offset: 48000, Polarity: - (NEG)
Trigger: GateLength: 1000, PreTrigger: 100, Threshold: 200
Slow Filter: IntTime: 350, FlatTop: 100, Tau: 25000
CLOVERS:
Input: InputRange: 2V, Impedance: 50Ohm, Offset: 50000, Polarity: - (NEG)
Trigger: Fast filter IntTime: 20, FlatTop: 20, Threshold: 30
Trigger: GateLength: 750, PreTrigger: 75
Slow Filter: IntTime: 500, FlatTop: 50, Tau: 37000 |
Attachment 1: 160718Conf_BrikenFull_cal5.xlsx
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57
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Wed Jul 20 17:18:59 2016 |
J.L. Tain, J. Agramunt, A. Tarifeño, A. Tolosa, K. Gabor, S. Go, K. Matsui... | Electronics |
Measurement with preamplifiers after drying.
Amplifiers are brought back after ~12h and connected.
Measurement of background for 1hour
Online: 160720_1350_1452_Bkg.root
Listmode: No
There might have been a slight improvement on the PA behaviour
but is not clear.
Attached a screen shot of the spectrum
The spurious signals show very little noise superimposed
as can be seen in the attached capture of the sample by the DACQ
but is not so obvious how this can help to veto them. |
Attachment 1: Bkg-afterPAdrying.png
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Attachment 2: V2A4C3-SpuriousSignal.png
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56
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Wed Jul 20 17:05:59 2016 |
J.L. Tain, J. Agramunt, A. Tarifeño, A. Tolosa, ... | Background |
Background measurement with remaining tubes (95) overnight
Listmode: 160719_2343_Bkg_*.dlt, Run: 031-044
Online: 160719_2343_1030_Bkg.root
Unfortunately the 252Cf source remained ind the hall (shielded and far away but still)
Screen shot of neutron spectrum |
Attachment 1: Bkg-with95tubes.png
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55
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Wed Jul 20 16:55:48 2016 |
K.Gabor, K. Matsui, A. Tarifeño | Electronic |
Drying of preamplifiers
PA8, PA9 and PA10 are removed and brought to a dryer box
to stay overnight and see if the situation with spurious signals
improves as suggested by Mesytec.
Extra drying in the morning with a hair dryer. |
54
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Wed Jul 20 16:50:12 2016 |
J.L. Tain, J. Agramunt, A. Tarifeño, A. Tolosa, S. Go... | 252Cf |
Measurement of the 252Cf source at the central position
Efficiency and neutron-gamma correlations
Listmode: 160719_2233_252Cf_XX.dlt, Run: 029-030
Online: 160719_2233_252Cf_029_030.root |
53
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Wed Jul 20 16:40:57 2016 |
S. Go, J.Agramunt, A.Tolosa, J.L. Tain,... | CLOVER |
Calibration and resolution check
CLOVER detectors were calibrated in energy with 60Co and 137Cs
60Co source: 2530, 8.81E4Bq (16/03/2010)
137Cs source: CD393 (box), ?
Sources were placed at the center
Resolution(FWHM@1333keV):
G7 Blue:2.67keV
G7 Green: 2.84keV
G7 Red: 2.77keV
G7 Black: 2.64keV
D4 Blue: 3.60keV
D4 Green: 3.35keV
D4 Red: 3.41keV
D4 Black: 4.85keV (!?)
Efficiency calibration with 152Eu
Source place at the center
Source: 272 (09-7011), 1.062E4Bq (error:1.9%)@16/03/2010
File: 160719_2201_152Eu_028.dlt
Online: 160719_2201_152Eu_028.root
Attached 152Eu spectrum |
Attachment 1: 152Eu.png
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52
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Wed Jul 20 16:12:58 2016 |
S. Go, ... | CLOVER |
Mounting of the CLOVER detectors in position
CLOVER G7: right of beam
CLOVER D4: left of beam
G7 crystals:
Beam ->
Back view:
Red Blue
Green Black
D4 crystals:
Beam ->
Front view:
Red Green
Blue Black
Photos of the arrangement with COVER detectors attached |
Attachment 1: DSC_2522.JPG
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Attachment 2: DSC_2523.JPG
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Attachment 3: DSC_2524.JPG
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51
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Wed Jul 20 16:07:58 2016 |
A.Tarifeño, J.L. Tain, J. Agramunt, A. Tolosa, ... | 252Cf |
19/Jul/2016
Scanning of the efficiency as a function of longitudinal position
File:160719_BRIKEN_252Cf_XXmm_*.dlt
Online:160719_BRIKEN_252Cf_XXmm.root
Run: 011-025
Distances: -275,-175,-125,-75,-50.-25,+25,+50,+75,+125,+175,+225,+275,+375mm |
50
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Wed Jul 20 12:00:15 2016 |
J.L. Tain, J. Agramunt, A. Tarifeño, A. Tolosa, ... | 252Cf |
Measurement with the source at the center
Listmode: 160719_BRIKEN_252Cf_009.dlt
Online: 160719_BRIKEN_252Cf.root
BRIKEN: 1.03697E7
Pulser: 5985
Rate: 17326 n/s |
49
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Wed Jul 20 11:49:00 2016 |
J.L. Tain, J. Agramunt, R. Baeturia, A. Tarifeño, A. Tolosa, ... | Background |
18/07/2016
First background measurement overnight.
START: 23:37
File: 160718_FullBrikenFirstData_bkg_*.dlt Run:003-006
Online: 160718_FullBrikenFirstData_bkg.root
Attached screenshots of raw data for every digitizer.
The problem of some of the PA is visible in the background
spectra.
In addition one can see in some of the channels signals
distributed over all the region up to the pulser and beyond.
This we found to be related to a too low threshold
but can be eliminated with a better adjustment. |
Attachment 1: 160718_FullBrikenFirstData_bkg.zip
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48
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Wed Jul 20 11:40:00 2016 |
J.L. Tain, J. Agramunt, R. Baeturia, A. Tarifeño, A. Tolosa, ... | 252Cf |
First measurement with full 140 tube version
of the BRIKEN neutron detector
Directory: /data/160716Test01/
Configuration: 160718Conf_BrikenFull.xlsx
File: 160718_FullBrikenFirstData_252Cf_002.dlt
Online: 160718_FullBrikenFirstData_252Cf.root
All tubes and channels working!
Sample of screenshots included. |
Attachment 1: RIKEN-252Cf-V1A1.png
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Attachment 2: UPC-252Cf-V1A3.png
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Attachment 3: ORNL1-252Cf-V1A5.png
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Attachment 4: ORNL2-252Cf-V1A6.png
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47
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Wed Jul 20 11:16:18 2016 |
J.L. Tain | Electronics |
Pulser settings
We use two pulsers, Pulser1 for RIKEN, ORNL1 and ORNL2 tubes (7 PA)
and Pulser2 for UPC tubes due to the different gains (3 PA)
10HzClock->G&DG->Pulser->LinearFI/FO
Pulser1: BNC BH-1: trise=1us, tfall=1ms, amp=670mV(scope), NEG
Pulser2: BNC PB-5: tfall=1ms, amp=0.180mV(setting), 90mV(scope), NEG
Later on we found out that Pulser1 is compatible also for
the CLOVER detectors (8PA). This will require an additional LinearFI/FO |
46
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Wed Jul 20 08:58:13 2016 |
J.L. Tain, I.Dillman, R. Caballero, J. Agramunt, A. Tarifeño, A. Tolosa, ... | Electronics |
Distribution of connections of tubes in preamplifiers and digitizers
Because of the need to use 10 PAs instead of 9 PAs we had to redistribute
the signal connections. Now:
PA1(RIKEN), PA2(RIKEN), PA3(UPC), PA4(UPC), PA5(UPC) -> V1A1-V1A4
PA6(ORNL1) -> V1A5
PA7(ORNL2) -> V1A6
PA8(ORNL2) -> V2A1,V2A2
PA9(ORNL2) -> V2A3,V2A4
PA10(ORNL2) -> V2A5,V2A6
So V1A1 to V1A4 contain now signals from 2 PAs.
We also redistributed the tubes within the PAs
We also changed the numbering or RIKEN Tubes. Tube 1 to 12 are now
those on the AIDA side (PA1 attached to the PE block)
A figure showing the distribution of tubes an numbering is included.
Tube 1 is behind tube 19 and so forth.
Attached also is an excel file with tube-channel distribution |
Attachment 1: TubeDistribution-new.xlsx
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Attachment 2: TubeDistribution-new.pdf
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45
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Tue Jul 19 13:47:55 2016 |
A. Tarifeño-Saldivia | Neutron efficiency - Scanning on Z preliminary result |
We have carried out a scanning of the neutron efficiency with respect to the position along the Z-axis (AIDA and BEAM hole) of a 252Cf neutron source. A preliminary analysis is presented based on data from the online. A plot with the comparison of the simulations and experimental data is attached. The experimental results are in good agreement with the GEANT4 simulations of the studies for design of the neutron detector. The simulations for the design of the hybrid mode were calculated using 148 3He counters. The version of the hybrid detector assembled during the current campaign (July-2016) is using 140 3He counters. The missing counters correspond to tubes located on the outer part of PE, thus the effect of these counters on the total neutron efficiency is minimal.
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Attachment 1: Preliminar_Zscaning_BRIKEN_PremLabel_vsmall.png
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44
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Tue Jul 19 11:54:03 2016 |
JL Tain A Tolosa R. Caballero A. Tarifeño J. Agramunt | Photos of the AIDA insertion hole with the 3He tubes |
RIKEN tubes on the AIDA side with the SHV right angle connector will protrude
by ~95mm in the HYBRID configuration (with CLOVERS).
In the current AIDA DSSD configuration there are six detectors occupying 45-50mm
at a distance to center of the stack from the black plastic support of ~430mm.
The hole for the CLOVER is 110mm. The center of the hole is at 375mm from the
PE end.
This means that the center of the current stack is only ~15mm beyond the PE
in the CLOVER hole, so 1 or 2 of the DSSD will be partially shadowed
from the CLOVER detectors.
(This do not represent any problem from the neutron detector point of view) |
Attachment 1: DSC_2520.JPG
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Attachment 2: DSC_2517.JPG
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Attachment 3: DSC_2515.JPG
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43
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Tue Jul 19 04:34:57 2016 |
JL Tain A Tolosa R. Caballero A. Tarifeño J. Agramunt | Photos of the electronics |
Racks, crates, rear part of the preamps and matrix with all tubes. |
Attachment 1: DSC_0034.JPG
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Attachment 2: DSC_0022.JPG
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Attachment 3: DSC_0016.JPG
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Attachment 4: DSC_2483.JPG
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Attachment 5: DSC_2497.JPG
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Attachment 6: DSC_2511.JPG
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Attachment 7: DSC_2513.JPG
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Attachment 8: DSC_2514.JPG
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Attachment 9: DSC_2526.JPG
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42
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Tue Jul 19 04:09:32 2016 |
JL Tain A Tolosa R. Caballero A. Tarifeño J. Agramunt | Last tube fit in the matrix!!! |
The photo of great moment |
Attachment 1: DSC_2478.JPG
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41
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Tue Jul 19 03:19:34 2016 |
A. Tarifeño, I. Dillman, J. Agramunt, A. Tolosa, J.L. Tain... | Electronics |
Preamplifier and signal cable testing
We check all signal cables,the flat cable connector to BNC
from ORNL/UTK and they are OK.
While checking the preamplifiers (PA) we realized that on the oscilloscope
some of the channels shown pulses without a load when HV is on.
After some checks, we come to the conclusion that is a kind of discharge
on the HV part of the preamp (which appears as positive pulse or negative pulses)
and induce pulses of opposite sign in one or mos neighbouring channels.
After systematically investigating them in the scope, we plug them in the DACQ
to record the spectra. For this we include an additional digitizer SIS3316
to connect al1 channel preamps
PA1(D):UPC:SN-0808223 -> V1A1
PA2(D):GSI:SN-1112572 -> V1A2
PA3(D):UPC:SN-0310315 -> V1A3
PA4(D):UPC:SN-0808220 -> V1A4
PA5(U):UTK: ? -> V1A5
PA6(U):UTK:SN-0808218 -> V1A6
PA7(U):UTK:SN-0713586 -> V1A7
PA8(U):UTK:SN-0808221 -> V2A1, V2A2
PA9(U):UTK:SN-0808215 -> V2A3, V2A4
PA10(U):UTK:SN-0808217 -> V2A5, V2A6
We measure first with a tube of each type connected to Ch#1 of each PA
to adjust parameters of digitizers and range
List-mode: 160717_preampCheck_000.dlt
On-line: 160717_preampCheck.root
Then we remove the tube from Ch#1 to see the effect in this channel:
List-mode: 160717_preampCheck_noTubes_001.dlt
On-line: 160717_preampCheck_noTubes.root
We attach screenshots for both as compressed files (.zip)
and the root files |
Attachment 1: preampCheck.zip
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Attachment 2: noTubeCh1.zip
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Attachment 3: 160717_preampCheck.root
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Attachment 4: 160717_preampCheck_noTubes.root
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40
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Mon Jul 18 19:01:36 2016 |
J.L. Tain | 3He tubes |
Adjustment of HV and PA gain
We adjust the HV for each tube type and the gain of the preamplifier (PA) in order
to have a similar signal amplitude for the 764keV peak in all of them.
Because of the very different gain between tubes we are not able to combine in the same
PA tubes from RIKEN and UPC, thus we have to go for 10 PA instead of 9:
Settings: Preamp (type), Tube type, HV, Gain, height or 764keV pulse, pulse polarity
PA1 (D), RIKEN, 1450V, LowGain, ~400mV, POS
PA2 (D), RIKEN, 1450V, LowGain, ~400mV, POS
PA3 (D), UPC, 1550V, HighGain, ~400mV, POS
PA4 (D), UPC, 1550V, HighGain, ~400mV, POS
PA5 (U), UPC, 1550V, HighGain, ~600mV, NEG
PA6 (U), ORNL1, 1200V, LowGain, ~400mV, NEG
PA7 (U), ORNL2, 1750V, LowGain, ~400mV, NEG
PA8 (U), ORNL2, 1750V, LowGain, ~400mV, NEG
PA9 (U), ORNL2, 1750V, LowGain, ~400mV, NEG
PA10 (U), ORNL2, 1750V, LowGain, ~400mV, NEG
We need to use two different pulse generators to adjust differently the pulse height
of UPC tubes |
39
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Mon Jul 18 18:40:32 2016 |
A. Tarifeño-Saldivia and J. L. Tain | 3He tubes - Testing |
Test of individual 3He tubes
The tests were done using the ATOMKI MCA and
HV: ISEG NH204M
Preamp: Mesytec MHV-16 (Unipolar IFIC)
Amp: ORTEC671 (Gain=5x0.5,SHP=6us)
Pulser: 10Hz-Clock + TC410A G&DG + BH-1 (tr=1us,tf=1ms,amp=0.7)
Spectra measured with 1024 channels
Counting time: 100s (UPC, RIKEN and ORNL 1")
120s (ORNL 2")
Neutron source: 252Cf
PE setup: 1 inches tubes were tested on the BELEN-20 PE matrix, while for 2 inches tubes a moderator was prepared
using existing material (see attached figures).
Attached a figure with a sample spectrum for each tube type
and a compressed file with all the measured spectra in ASCII format.
All the tubes performed correctly. The neutron signal is well separated from the noise.
The RIKEN tubes have the highest gain. Gain in the UPC tubes is the lowest.
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Attachment 1: Histograms_testing_BRIKEN_tubes_Jul16.zip
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Attachment 2: Tube1_RIKEN.png
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Attachment 3: Tube25_UPC.png
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Attachment 4: Tube65_ORNL_1inch.png
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Attachment 5: Tube88_ORNL_2inch.png
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Attachment 6: setup_1inch.jpeg
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Attachment 7: setup_2inch.jpeg
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38
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Mon Jul 18 09:32:50 2016 |
Shintaro Go | HV controls |
You can start applying HVs on the detectors using macro on the control-computer.
If you have already signed in the computer that controls mpod,
1. Type http://192.168.13.239/ to monitor the status of HV.
2. Go to the directory : /home/pixie16/DAQ_1/include and open the config file : hvmon.conf
Type IP address channel slot name voltage Current RampUp RampDn Switch On/Off/RESET
V A V/s V/s 1 / 0 / 10
------ --------------- --------- ----- ---- ------- ------- ------ ------ -------------
0 192.168.13.239 0 0 PA1 1450 0.0001 50 10 0
0 192.168.13.239 1 0 PA2 1450 0.0001 50 10 0
0 192.168.13.239 2 0 PA3 1550 0.0001 50 10 0
0 192.168.13.239 3 0 PA4 1550 0.0001 50 10 0
0 192.168.13.239 4 0 PA5 1550 0.0001 50 10 0
0 192.168.13.239 5 0 OFF 0 0.0001 50 10 10
0 192.168.13.239 6 0 OFF 0 0.0001 50 10 10
0 192.168.13.239 7 0 OFF 0 0.0001 50 10 10
0 192.168.13.239 0 1 PA6 1200 0.0001 50 10 0
0 192.168.13.239 1 1 PA7 1750 0.0001 50 10 0
0 192.168.13.239 2 1 PA8 1750 0.0001 50 10 0
0 192.168.13.239 3 1 PA9 1750 0.0001 50 10 0
0 192.168.13.239 4 1 PA10 1750 0.0001 50 10 0
0 192.168.13.239 5 1 OFF 0 0.0001 50 10 10
0 192.168.13.239 6 1 OFF 0 0.0001 50 10 10
0 192.168.13.239 7 1 OFF 0 0.0001 50 10 10
0 192.168.13.239 0 3 D40 3000 0.0001 2 5 0
0 192.168.13.239 1 3 D41 3000 0.0001 2 5 0
0 192.168.13.239 2 3 D42 3000 0.0001 2 5 0
0 192.168.13.239 3 3 D43 3000 0.0001 2 5 0
0 192.168.13.239 4 3 G70 2500 0.0001 2 5 0
0 192.168.13.239 5 3 G71 3000 0.0001 2 5 0
0 192.168.13.239 6 3 G72 2500 0.0001 2 5 0
0 192.168.13.239 7 3 G73 2500 0.0001 2 5 0
When you want to start HVs, you may have to change the last bit to be 1.
Then go to the following path /home/pixie16//DAQ_1/hv-mpod and execute the command ./hvmon (The process should start),
When you want to down HVs, you may have to change the last bit to be 1.
Sometime you may get error messages colored red on the status monitor when you down the HVs, then you have to change the config file (hvmon.conf) and set the last bit to be 10 to clear the error messages.
--------------------------------------
The IP adress of the computer is currently 192.168.13.250. The user name : pixie16, password: ask Nathan or Shintaro
For now, slot names PA should be He3 and DXX and GXX should be clovers.
You can also change the HV values by changing hvmon.conf
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37
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Fri Jul 15 11:47:31 2016 |
Nathan Brewer and Alvaro Tolosa | Preliminary Ge Calibration, Resolution and Configuration |
Today several tests (3) were done with the germanium detectors with the voltage configuration listed in the previous entry.
The tests were as follows:
Tests with 60Co+137Cs sources
1. Initial evaluation of calibration and resolution (Calibration60Co137Cs_energySignal.root)
2. Cable changes to optimize resolution for detector D4 (Calibration60Co137Cs_timingSignal.root)
Test with 152Eu
3. Final (proposed) configuration of filter parameters, voltages, and cable connections. (Calibration152Eu.root)
------------------------------------------------------------------------------------------------------------------------------------
At the time of this log the evaluation of resolution and calibration based on Eu data is to be completed.
The configuration file for the Ge is listed in FirsttestGe.xlsx .
The details of the tests can be found in the attached .pdf pictures or in the .root files.
You may notice that 2/4 of each clover count less than the other 2 and this is due to source position.
For the runs on Co and Cs It was seen that D4 had considerable tailing in channels 1 and 3 (black and green leaves, respectively) and D4 has worse resolution. Channel 3 (green) also requires a non-linear calibration. Currently only linear calibration is applied. But this is as expected from how the detectors were running before leaving Tennessee.
Therefore we decided to check if the second group of signal cables had better resolution for detector D4. The second group of cables were presumed to be timing signals and the run is labeled as such, however, the signals are similar within a few percent and this assumption may have been incorrect.
The result is listed in calibrationClovers.ods in the third tab (TimingvsEnergy).
!!!Noise in the different groups of cables should be evaluated.!!!
Based on this test the first cable from the first test in D4 was reattached and the others remain in place. The second channel saw improvement and the 3rd and 4th channels saw limited change (deemed insignificant). This bundle has been labeled 'D4 Signal' for now.
Avg. D4 Resolution for Co and Cs lines is 3.3 keV FWHM
Avg. G7 Resolution for Co and Cs lines is 2.6 keV FWHM
We estimate that these are accurate within ~10%. But this is sufficient analysis for this point and time.
Further details will be posted regarding the Eu data , at a glance the configuration is seen to be very close except for the known non-linearity in D4 and one channel from G7 which should definitely be recalibrated. Thresholds and noise levels should also be re-evaluated.
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Attachment 1: D4_CoCs_71516.pdf
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Attachment 2: D4_Eu_71516.pdf
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Attachment 3: G7_CoCs_71516.pdf
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Attachment 4: G7_Eu_71516.pdf
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Attachment 5: Calibration60Co137Cs_energySignal.root
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Attachment 6: Calibration60Co137Cs_timingSignal.root
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Attachment 7: Calibration152Eu.root
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Attachment 8: calibrationClovers.ods
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Attachment 9: FirsttestGe.xlsx
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36
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Fri Jul 15 08:29:14 2016 |
Nathan Brewer, Shintaro Go | Expected Performance and Voltage Setting for Germanium |
Expected Resolution:
------------------------------
G7 should be ~2.0 keV FWHM at 600 keV for all crystals.
D4 should be as low as 1.8 and as high as 3.3 keV FWHM at 600 keV.
Configuration File: (~/DAQ_1/include/hvmon.conf)
-----------------------------------------------------------------
Type IP address channel slot name voltage Current RampUp RampDn Switch On/Off
V uA V/s V/s 1/0
------ --------------- --------- ----- ---- ------- ------- ------ ------ -------------
0 192.168.13.239 0 3 D40 3000 0.5 2 5 1
0 192.168.13.239 1 3 D41 3000 0.5 2 5 1
0 192.168.13.239 2 3 D42 3000 0.5 2 5 1
0 192.168.13.239 3 3 D43 3000 0.5 2 5 1
0 192.168.13.239 4 3 G70 2500 0.5 2 5 1
0 192.168.13.239 5 3 G71 3000 0.5 2 5 1
0 192.168.13.239 6 3 G72 2500 0.5 2 5 1
0 192.168.13.239 7 3 G73 2500 0.5 2 5 1
In all cases (Temperature Monitor, ACQ, etc.) D4 comes before G7 and in the same order.
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35
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Sat Jul 9 21:26:25 2016 |
J.L. Tain | EDACQ |
Electronics and DACQ for July 2016 assembly: hardware and connections |
Attachment 1: EDACQ-July2016.pdf
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34
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Sat Jul 9 21:21:38 2016 |
J.L. Tain | 3He tubes |
Tube distribution in the moderator, pre-amplifiers and digitizers |
Attachment 1: TubeDistribution.pdf
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Attachment 2: TubeDistribution.xlsx
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33
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Sat Jul 9 21:14:12 2016 |
J.L. Tain | 3He tubes |
Drawings and specs of 3He tubes |
Attachment 1: He3_GE_30cm-RIKEN.pdf
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Attachment 2: 1inch3He-ORNL.pdf
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Attachment 3: 2inch3He_ORNL.pdf
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Attachment 4: He3-252248-UPC-GSI.pdf
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32
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Sat Jul 9 21:08:08 2016 |
J.L. Tain | Neutron moderator |
Drawings of the polyethylene neutron moderator and table assembly |
Attachment 1: Moderator-Table.pdf
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Attachment 2: Table.pdf
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Attachment 3: Moderator-Shielding.pdf
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31
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Sat Jul 9 21:00:54 2016 |
J.L. Tain | Hardware |
A list of the available hardware |
Attachment 1: Hardware.xlsx
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Attachment 2: Hardware.pdf
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30
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Sat Jul 9 20:44:31 2016 |
J.L. Tain | BRIKEN neutron detector |
START
Assembly and commissioning of BRIKEN neutron detector
The hybrid configuration of the BRIKEN neutron detector will be assembled at BF2 for the first time with 140 3He
tubes and 2 CLOVER detectors, connected to the Gasific digital data acquisition system and tested with 252Cf
sources. |
29
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Mon May 11 09:14:54 2015 |
G. Kiss | 252Cf_data_sheet |
The activity of the 252Cf source, used for the calibration was 3.7 MBq at 15.05.2006. Unfortunately, uncertainty is missing from the data sheet :-( |
28
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Fri May 8 03:20:48 2015 |
J.Agramunt J.L.Tain K.Gabor | BnCorrelation |
We run all the night until the end of beam time, and the Bn correlations are more clear now. |
Attachment 1: BnCorr.pdf
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27
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Thu May 7 08:36:56 2015 |
J.L. Tain, J. Agramunt, A. Estrade, G.Kiss, T. Davinson, C.Griffin | First BRIKEN_v.0 beta-delayed neutron correlations? |
During the 98,100Kr setting run we observe
in the time correlation plot (middle right panel)
of beta signals (marked by AIDA, with amplitude larger than ch=600)
with Riken 3He tube signals (noise and pulser cleaned)
a small peak around t=0 which might be indication
of beta-delayed neutrons.
The spectrum was measured for about 2h. |
Attachment 1: Screenshot_from_2015-05-07_16_01_27.png
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26
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Wed May 6 11:41:24 2015 |
J. Agramunt, A. Estrade | First online combined analysis |
Screen shot of the rudimentary on-line
analysis of the combined data:
BRIKEN-AIDA-BigRIPS
Top Left: dE (from MUSIC) vs. ToF (F11-F7)
Top Right: X-position (at F9) vs ToF
Middle Left: Amplitude spectrum of RIKEN tubes
Bottom Left: Energy spectrum from AIDA marked as beta-decays
Middle Right: Time correlations between betas (AIDA) and neutrons (BRIKEN)
Bottom Right: Time correlations between implants (AIDA) and neutrons (BRIKEN)
(the range of time correlated data [-1ms,+1ms]) |
Attachment 1: Screenshot_from_2015-05-06_19_12_29.png
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25
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Wed May 6 05:10:14 2015 |
J.L. Tain, J. Agramunt, G. Kiss | 94Se setting measurement |
After the long shutdown the beam is back at 00:30 (06/05)
Intensity is slightly lower 26pnA and somewhat unstable (short time)
Measurement in the morning:
File: 150506_0846_0915_94Se.root
Average rate per tube (n/s): U=3.39 D=0.93B=0.40
Notes:
-The rate has increased by 3.5 in the detectors close to EURICA (!?)
-The rate at the detector below the MUSIC is substantial.
From the different magnitudes it is clear that neutrons are originated
both outside and inside EURICA. |
24
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Wed May 6 04:57:24 2015 |
J.L. Tain, J. Agramunt, G. Kiss | New degrader thickness |
The Al degrader thickness was reduced to 4.8mm |
23
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Tue May 5 05:29:26 2015 |
J.L. Tain, J. Agramunt, G. Kiss | Ambient background measurement |
Beam still down. New background measurement
with new RIKEN tube below the MUSIC chamber
(call it B)
File: 150505_0040_1130_aprox_bckg.root
Average rate per tube (n/s): U=0.0073, D=0.0065, B=0.0070 |
22
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Tue May 5 05:17:36 2015 |
J.L. Tain, J. Agramunt, G. Kiss | Ambient background measurement |
Failure of a quadrupole triplet at BigRIPS (some time after earthquake)
We take the chance of measuring background:
File: 150504_1500_2047_bckg.root
Rate per tube (n/s): U=0.098, D=0.0062, US=0.0200
Ratio to 1st 110Zr: U=1.38, D=1.99, US=0.90
Notes:
-Compared to the 1st background measurement there are changes
larger than expected statistical fluctuations:
perhaps due to slight changes in noise
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21
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Tue May 5 05:04:00 2015 |
J.L. Tain, J. Agramunt, G. Kiss | Change of degrader thickness |
For EURICA measurements degrader thickness were increased
trying to decrease MACI and AIDA trigger rate
Before we had 5.7 mm of Al
Now we have:
Degrader: 4.0 + 1.0 + 0.6 + 0.4 +0.3 = 6.3 mm of Al
also 2x 0.8mm Al plates were added before
the MACI start detector (thus covering partially AIDA)
Trigger from AIDA will be taken from 3rd DSSSD |
20
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Tue May 5 02:19:58 2015 |
j.Agramunt J.L.Tain K.Gabor | The Lower polyethylene pieces was swamped |
The Lower polyethylene pieces was swamped.
In the photo beam comes from the left.
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Attachment 1: photo-4.JPG
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19
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Mon May 4 15:03:47 2015 |
J.Agramunt J.L.Tain K.Gabor | New detector placed under the beam line |
New detector placed under the beam line, below MUSIC chamber
This detector replace the USA tubes in the DACQ because we need the preamp to plug it.
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Attachment 1: photo_2-2.JPG
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Attachment 2: photo_1-2.JPG
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Attachment 3: photo_3-2.JPG
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18
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Mon May 4 04:14:18 2015 |
J.Agramunt J.L.Tain K.Gabor | AIDA trigger plugged in Mod2 Ch12 |
AIDA trigger plugged in Mod2 Ch12 |
17
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Mon May 4 03:20:00 2015 |
Shunji Nishimura | RNC New Rule |
We have some new rule about the data taken at RNC from this year.
Shunji
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Attachment 1: kanri_e.pdf
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16
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Mon May 4 02:36:16 2015 |
J.Agramunt J.L.Tain K.Gabor | Maki trigger plugged in Mod2 Ch9 |
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15
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Mon May 4 02:26:14 2015 |
J.Agramunt J.L.Tain K.Gabor | F11 trigger plugged in Mod2 Ch16 of Briken daq |
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14
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Sun May 3 10:10:13 2015 |
J.L. Tain, J. Agramunt, G. Kiss | 94Se setting measurement |
94Se setting:
File: 150503_1500_1554_94Se.root
Rate per tube (n/s): U=0.966, D=0.263, US=0.538
Ratio to 1st 110Zr: U=2.00, D=1.89, US=1.84
Notes:
-Compared to the 1st 94Se setting measurement (12:19-13:19)
there is a drop of 25% in the rate without apparent reason |
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Sun May 3 10:07:25 2015 |
J.L. Tain, J. Agramunt, G. Kiss | Photos of new PE shielding |
Photos of the general arrangement and details of the new PE blocks |
Attachment 1: 20150502_195020.jpg
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Attachment 2: 20150502_194340.jpg
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Attachment 3: 20150502_192253.jpg
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Sun May 3 09:04:07 2015 |
J.L. Tain, J. Agramunt, G. Kiss | Summary of neutron measurements |
U: (Up: 2 RIKEN tubes at 40cm from AIDA)
D: (Down: 12 RIKEN tubes at 80cm from AIDA)
US: (2 ORNL 2" tubes close to the floor at 1.8m from AIDA)
Natural background:
File: 150426_Bckg_1425_1805.root
Rate per tube (n/s): U=0.0071, D=0.0045, US=0.0222
Notes:
-This rate seems quite small but we should remember
that we are underground.
-The fact that U is larger than D could be explained as
related that the amount of PE around tubes is larger.
-For comparison:
BELEN-20@JYFL=0.6n/s (no beam), 0.9n/s (beam)
BELEN-30@GSI=1.2n/s (beam)
BELEN-48@JYFL=1.5n/s
110Zr setting:
File:150501_16111810_110Zr.root
Rate per tube (n/s): U=0.483, D=0.139, US=0.292
Ratio to background: U=68.3, D=31.1, US=13.2
Individual tube distribution:
U1 0.280 D1 0.087 D7 0.084 US1 0.132
U2 0.249 D2 0.092 D8 0.084 US2 0.188
D3 0.083 D9 0.077
D4 0.075 D10 0.070
D5 0.073 D11 0.069
D6 0.065 D12 0.054
Notes:
-There is huge increase of with beam
-The drop of increase with distance is consistent
with either beam induced or decay of implants
110Zr setting:
File: 150501_1733_1900_110Zr.root (actually 02/05)
Rate per tube (n/s): U=0.869, D=0.242, US=0.516
Ratio to 1st 110Zr: U=1.80, D=1.74, US=1.77
Notes:
-We don't quite understand the reason for the near factor two
difference since apparently the settings are the same and beam was
rather stable
In order to investigate the point of origin of the neutrons
we add extra PE covering D5,D6,D11,D12 from the top and
D1,D2,D7,D8 from the front
88Ge setting:
File: 150502_21502333_88Ge.root
Rate per tube (n/s): U=1.271, D=0.349, US=0.706
Ratio to 1st 110Zr: U=2.63, D=2.51, US=2.42
Individual rates:
U1 1.340 D1 0.424 D7 0.402 US1 0.576
U2 1.202 D2 0.446 D8 0.381 US2 0.835
D3 0.408 D9 0.342
D4 0.393 D10 0.315
D5 0.359 D11 0.250
D6 0.275 D12 0.193
Notes:
-One notices a relative drop of rate for D6, D11 and D12
pointing to a source located in the vicinity of AIDA
94Se setting:
File: 150503_1219_1319_94Se.root
Rate per tube (n/s): U=1.267, D=0.349, US=0.717
Ratio to 1st 110Zr: U=2.62, D=2.51, US=2.46
Notes:
-Very similar to 88Ge measurement |
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Sat May 2 19:32:08 2015 |
AE | transfer data AIDA->BRIKEN |
A test program for online data transfer is available in aidas1 PC at:
/homes/npg/aev/AIDAbriken/AIDA-jorge-san.exe
no arguments are required to run it from command line |
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Sat May 2 03:52:14 2015 |
J.L. Tain | 3He tube description |
3He tube drawings and technical details:
RIKEN, UPC, GSI, ORNL-1, ORNL-2 |
Attachment 1: He3_GE_30cm.pdf
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Attachment 2: He3-252248.pdf
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Attachment 3: 1inch3He.pdf
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Attachment 4: 2inch3He.pdf
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Mon Apr 27 10:18:21 2015 |
K.Gabor S.Nishimura J.Agramunt | ORNL 3He tube at RIKEN |
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Attachment 1: photo-3.JPG
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Mon Apr 27 04:40:43 2015 |
G. Kiss, J. Agramunt | neutron background at Eurica |
Based on an about 8h long background measurement, the neutron background at the Eurica site was found to be about 0.006 neutron / sec (in the Riken tubes) and 0.019 neutron / sec (in the ORNL tubes). The beam was OFF. |
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Sat Apr 25 08:25:42 2015 |
G. Kiss, J. Agramunt | BRIKEN Test setup |
Altogether 16 tubes are mounted for the parasitic detector test (see the attached photos):
- two tubes (belonging to RIKEN) are in a 10 cm x 10 cm x 30 cm polyethylene matrix inside Eurica, the distance from AIDA is about 30 cm
- 12 tubes (belonging to RIKEN) are in a 20 xm x 30 xm x 30 cm matrix, outside (below) Eurica, at the closest possible place to AIDA, the distance is about 60 cm
- further two tubes (ORNL) are at the bottom of the Eurica support, about 1.2 m from the AIDA Silicon.
Furthermore, spectra measured using a 252Cf source is attached to this report, too (Jap1Cf-RIKEN tube, Us1Cf-ORNL tube). At the moment a background measurement is running. |
Attachment 2: P1120023.JPG
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Attachment 3: Jap1Cf.pdf
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Attachment 4: US1Cf.pdf
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Wed Feb 25 07:38:42 2015 |
A. Estrade J. Agramunt | Usage of synchronization test programs |
In order to access to the synchronization test, we prepare two programs in the PC briken1 ( 10.32.6.54).
To Launch the processes, in a terminal type: DataSink -i 3
In other terminal type SynCheck
By default this preform a test with difference RIBF-BRIKEN and AIDA-BRIKEN.
In case of BRIKEN is not running, the option "SynCheck -M 1" perform de differences AIDA-RIBF and BRIKEN-RIBF, and "SynCheck -M 2" RIBF-AIDA and BRIKEN-AIDA
AIDA Data Relay:
The programming transmitting the data from AIDA to the DataSink includes an intermediate filtering step. This selects only correlation scalars from one module (and possibly ADC values from one channel in that module).
To run the program from aidas1 PC:
DataRelayFilter -n 10.32.6.54 -p 10307 -I 2
"-I 2" selects ID 2 as the one for the AIDA data stream, which must correspond to the one expected by the DataSink in the briken1 PC.
The attached screenshot show the terminal when running the code in verbose mode (-v 1), and also sending the ADC energy of the pulser in channel 10 of NNAIDA11 (adc ~38600 ch). This was for random pulser; for a fixed pulser delta will show constant value of delta (timestamp difference between consecutive correlationpulses).
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Attachment 1: 15.png
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Attachment 2: DataRelayFilter_terminal.png
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Tue Feb 24 09:34:54 2015 |
J. Agramunt, H. Baba, A. Estrade | [DAQ] DAQ correlation test |
We have performed a successful test of the integration of independent DAQ systems based on a correlation
scalar counted from a common clock signal. The principles of the integration method are described in the
following AIDA elog entry: https://elog.ph.ed.ac.uk/AIDA/29
The configuration of the setup we used in the RIKEN test is described by the attached figure:
DAQcorrelation_diagram.pdf. The chosen solution was to use a 25 MHz clock generated by the MACB modules of
AIDA, which was distributed to the other two systems by a SIS36/38xx module in the BRIKEN VME crate (a
slightly modified versio of the method proposed by PCS in AIDA Elog#29).
The correlation can be monitored online using the MIDAS DataXfer and DataSpy toolkits
(http://npg.dl.ac.uk/MIDAS/DataAcq/Data.html). Each system operates a DataRelay program that sends a data
stream consisting only of IDs and time-stamps to a common DataSink (this requires a DataRelay code that
does
some filtering of the raw data). The scheme is shown in the attached diagram (DAQsoftware.pdf).
The DataPeek_Merge and SyncCheck codes use C++11 for parallelization of tasks, which is a helpful feature
to
improve the efficiency of finding coincidences between the correlation pulses. Thus, the code will not
run
in PCs with any Linux version. For example, it requires version 7 of ScientificLinux, which installed in
the
PC being used for BRIKEN DAQ control that will stay at RIBF for the time being.
++ SYNCHRONIZATION RESULTS ++
The figure correlation_25Hz.png shows a correlation plot for the BRIKEN+RIBF+AIDA running with
correlations
done by a pulser at 25 Hz. A large fraction of the pulsers appear in the double-coincidence plots (top
row;
same plots, except the 'Partial' one is automatically cleared every ~10seconds).
The bottom plots show the pair-wise correlations between BRIKEN and RIBF or AIDA. BRIKEN was defined as
the
'master' in this test, but current version of the program is flexible to select any stream as the master
one.
The second figure (correlation_random.png) shows the same test, but using a non-periodic pulser to trigger
the correlation scalar. We observed the same level of synchronization (peaks look broader because of the
zoom level). |
Attachment 1: DAQcorrelation_diagram.pdf
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Attachment 2: DAQsoftware.pdf
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Attachment 3: correlation_25Hz.png
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Attachment 4: correlation_random.png
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4
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Mon Feb 16 00:29:00 2015 |
Gabor KISS | Polyethyelene |
The polyethelene arrived at RIKEN. Except 4 neighboring holes (located at the inner ring) the alignment is OK. |
Attachment 1: bottom1.JPG
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Attachment 2: small2.JPG
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Fri Oct 31 12:58:49 2014 |
Robert Grzywacz | Entry test - preamps |
Here is a picture of one of our Mesytec preamplifiers. We have located all seven of them.
They have 16 input channels and a common SHV per board.
<p> <a href="141031_125516/24.png?lb=BRIKEN"><img border="0" alt="24.png" src="141031_125516/24.png?
lb=BRIKEN&thumb=1" name="att0" id="att0" /></a></p> |
Attachment 1: 24.png
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Fri Oct 31 11:36:57 2014 |
Alfredo Estrade | BRIKEN elog: take 2 |
A elog for the setup of the BRIKEN detector is now operational at https://elog.ph.ed.ac.uk/BRIKEN/
We have setup a list of emails that will receive automatic updates for each new entry to the logbook: C. Domingo, G. Lorusso, T. Davinson, A. Estrade, K. Rykaczewski, J.L. Tain, C. Griffin, S. Nishimura, I. Dillman, F. Montes, J. Agramunt, G. Cortes, F. Calvino, M. Marta
Please let us know the contact info for any other person that would like to be included in this list, or if you would like your email to be removed from it (should the new entries be too frequent for your inbox traffic!). |
1
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Fri Oct 31 09:47:59 2014 |
Alfredo Estrade | BRIKEN elog: Hello world! |
A elog for the setup of the BRIKEN detector is now operational at https://elog.ph.ed.ac.uk/BRIKEN/
We have setup a list of emails that will receive automatic updates for each new entry to the elog:
C. Domingo, G. Lorusso, T. Davinson, A. Estrade, K. Rykaczewski, J.L. Tain, C. Griffin, S. Nishimura, I. Dillman, F. Montes, J. Agramunt, G. Cortes, F. Calvino, M. Marta
Please let us know about any other person that would like to be included in this list, or if you would like your email to be removed from it (should the new entries be too frequent for your inbox traffic!).
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