ELOG BRIKEN

AIDA GELINA BRIKEN nToF CRIB ISOLDE CIRCE nTOFCapture DESPEC DTAS EDI_PSA 179Ta CARME StellarModelling DCF K40

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	ID	Date	Author	Subject
	12	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
	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.
	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
	358	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

	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

Attachment 2: spec_de_2.jpg

Attachment 3: IMG_1340.JPG

	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
	123	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
	145	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.
	321	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

Attachment 2: OfflineConf_Signals.csv
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
	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
	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
	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 !!!!
	63	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

Attachment 2: BRIKENfront.jpg

Attachment 3: AIDAback.jpg

Attachment 4: AIDAintoBRIKEN.jpg

Attachment 5: AIDAnosefront.jpg

Attachment 6: AIDA-CLOVERhole.jpg

	101	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
	131	Mon Nov 7 13:44:26 2016	Alvaro, Ale, Jorge, Jose	Running Gasific and run protocol
Preliminary
Attachment 1: GasificShort.pdf

	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

	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
	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:

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