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ID |
Date |
Author |
Subject |
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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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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 |
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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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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). |
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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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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 |
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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 |
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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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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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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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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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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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137
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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 |
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138
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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 |
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135
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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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350
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Wed Oct 25 18:12:43 2017 |
Sunflower collaboration | Gamma sources web page |
http://www.nishina.riken.jp/collaboration/SUNFLOWER/misc/util/ribfsource.html |
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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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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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233
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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 |
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226
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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. |