ID |
Date |
Author |
Subject |
134
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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
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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
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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
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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
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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
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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
|
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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