| ID |
Date |
Author |
Subject |
|
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
|
|
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 |
|
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
|
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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. |
|
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 |
|
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 |
|
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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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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210
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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
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348
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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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12
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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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308
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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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207
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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 |
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396
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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
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| Attachment 2: He086_Pulser_samples.png
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| Attachment 3: He001_Pulser_samples.png
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| Attachment 4: He001_NoPulser_samples.png
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| Attachment 5: He013_Pulser_samples.png
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| Attachment 6: He013_NoPulser_samples.png
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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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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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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:
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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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203
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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
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| Attachment 1: 1_top_60co.png
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| Attachment 2: 2_top_noiselvl.png
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| Attachment 3: 3_bottom_60co.png
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| Attachment 4: 4_bottom_noiselvl.png
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6
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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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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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