25 Feb 2006
First time we have beam.
Electron trigger(T2) rates dependence to BB Total Sum(TS) threshold values was measured, based on run 2195.
Current: 5uA
Threshold (mV / MeV) | 20 / 100 | 40 / 200 | 60 / 300 | ||||||
Rate (Hz) | 1.014 *106 | 5.980 *104 | 1.830 *104 |
Current: 2uA
Threshold (mV / MeV) | 60 / 300 | 80 / 400 | |||||||
Rate (Hz) | 7430 | 2800 |
Current: 10uA
Threshold (mV / MeV) | 80 / 400 | 100 / 500 | 120 / 600 | ||||||
Rate (Hz) | 1.5 *104 | 6200 | 2700 |
26-27 Feb 2006
DC VME crates was changed to FastBus? crates with.28 Feb 2006
BB HV was adjasted using elastic run 2429.
HV settings before adjastment:
/w/work3503/e02013/GEn/adaq.bk/adev/slowc/HV_BB/hv_set/bb_hv_28_02_2006.set
Hv settings after adjastment:
/w/work3503/e02013/GEn/adaq.bk/adev/slowc/HV_BB/hv_set/bb_hv_28_02_2006_adj2429.set
Adjastment factors based on run 2429:
/w/work3503/e02013/GEn/adaq.bk/adev/slowc/scripts/adj_sh_2429.dat - for Shower.
/adj_ps_l_2429.dat - for left PS.
/adj_ps_r_2429.dat - for right PS.
01 Mar 2006
Background rate calculation for different beam positions.
Run # | Target | Current (uA) | Time (sec) | Ax | Ay | Bx | By | Rate (Hz) | Rate per uA (Hz/uA) |
2461 | Reff cell empty | 1.194 | 290 | -0.221 | -1.451 | -0.352 | -0.751 | 0.328 | 0.275 |
2462 | Reff cell empty | 5.217 | 330 | -0.318 | -1.599 | -0.387 | -0.864 | 1.882 | 0.361 |
2463 | Reff cell empty | 0.625 | 325 | -0.274 | -1.333 | -1.493 | 0.478 | 0.185 | 0.296 |
2464 | Reff cell empty | 0.629 | 295 | -0.240 | -1.433 | -1.559 | -2.826 | 0.234 | 0.372 |
2465 | Reff cell empty | 0.628 | 305 | -0.263 | -1.297 | 0.880 | -0.920 | 0.262 | 0.417 |
2466 | Reff cell empty | 0.558 | 300 | -0.281 | -1.325 | 0.926 | 0.390 | 0.357 | 0.640 |
02 Mar 2006
Counting rates was calculated for Vacuum, HE3 and H2 targets, both for electrond and pions.
Based on runs 2461, 2473 and 2485.
Run # | Target | Current (uA) | Time (sec) | Ax | Ay | Bx | By | Electrons rate per uA (Hz/uA) | Pions rate per uA (Hz/uA) |
2461 | Vacuum | 1.194 | 290 | -0.221 | -1.451 | -0.352 | -0.751 | 0.275 | 0.436 |
2473 | He3 | 1.192 | 1837 | -0.215 | -1.639 | -0.347 | -0.817 | 4.551 | 3.194 |
2485 | H2 | 2.145 | 1826 | -0.268 | -1.659 | -0.354 | -0.809 | 4.416 | 2.994 |
03 Mar 2006
BB Scintillators time resolution study.
For scintillators 5 and 6 was ploted following distribution:
(LT5 + RT5)/2 - (LT6 + RT6)/2, where
LT - left PMT time, RT - right PMT time, numerical index - scintilator bar number.
Sigma for this distribution was 1.48ns.
Then same distribution was ploted with cut on scintillators amplitude value:
LA5>400 && RA5>400 && LA6>400 && RA6>400, where
LA - left PMT amplitude, RA - right PMT amplitude, numerical index - scintilator bar number.
Sigma for this distribution was 0.45ns.
Same calculations was made form all scintillator bars, combined into pairs:
1&2, 2&3, 3$4 ... 11&12, 12&13.
Scintillator bars | Distribution | Cuts | Sigma | Comment | |||||
1 & 2 | (LT1 + RT1)/2 - (LT2 + RT2)/2 | LA1>400 && RA1>400 && LA2>400 && RA2>400 | 0.55 | Small statistic | |||||
2 & 3 | (LT2 + RT2)/2 - (LT3 + RT3)/2 | LA2>400 && RA2>400 && LA3>400 && RA3>400 | 0.79 | Small statistic | |||||
3 & 4 | (LT3 + RT3)/2 - (LT4 + RT4)/2 | LA3>400 && RA3>400 && LA4>400 && RA4>400 | 0.50 | ||||||
4 & 5 | (LT4 + RT4)/2 - (LT5 + RT5)/2 | LA4>400 && RA4>400 && LA5>400 && RA5>400 | 0.57 | ||||||
5 & 6 | (LT5 + RT5)/2 - (LT6 + RT6)/2 | LA5>400 && RA5>400 && LA6>400 && RA6>400 | 0.45 | ||||||
6 & 7 | (LT6 + RT6)/2 - (LT7 + RT7)/2 | LA6>400 && RA6>400 && LA7>400 && RA7>400 | 0.51 | ||||||
7 & 8 | (LT7 + RT7)/2 - (LT8 + RT8)/2 | LA7>400 && RA7>400 && LA8>400 && RA8>400 | 0.66 | ||||||
8 & 9 | (LT8 + RT8)/2 - (LT9 + RT9)/2 | LA8>400 && RA8>400 && LA9>400 && RA9>400 | 0.62 | ||||||
9 & 10 | (LT9 + RT9)/2 - (LT10 + RT10)/2 | LA9>400 && RA9>400 && LA10>400 && RA10>400 | 0.62 | ||||||
10 & 11 | (LT10 + RT10)/2 - (LT11 + RT11)/2 | LA10>400 && RA10>400 && LA11>400 && RA11>400 | 0.49 | ||||||
11 & 12 | (LT11 + RT11)/2 - (LT12 + RT12)/2 | LA11>400 && RA11>400 && LA12>400 && RA12>400 | 0.44 | ||||||
12 & 13 | (LT12 + RT12)/2 - (LT13 + RT13)/2 | LA12>400 && RA12>400 && LA13>400 && RA13>400 | 0.50 |