strutture:lnf:da:btf:dispositivi:rivelatori:calorimeter:cherenkov
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strutture:lnf:da:btf:dispositivi:rivelatori:calorimeter:cherenkov [2022/05/16 08:11] – foggetta@infn.it | strutture:lnf:da:btf:dispositivi:rivelatori:calorimeter:cherenkov [2022/12/21 16:19] (current) – foggetta@infn.it | ||
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+ | ======CALOBTF1====== | ||
+ | \\ | ||
+ | **Lead Glass -> Cherenkov**\\ | ||
+ | \\ | ||
+ | From the former OPAL electromagnetic calorimeter\\ | ||
+ | **Referred measuring System**\\ | ||
+ | Caen V965 - CH4 900pC (old Type)\\ | ||
+ | Caen N625 - CH2 @ -7mV bias\\ | ||
+ | |||
+ | |||
+ | \\ | ||
+ | **N=184.85*(x)^7.705*Ebeam\E0** \\ | ||
+ | N = single particle value [adc unit, pedestal subtracted]\\ | ||
+ | x = V/1200 [V]\\ | ||
+ | V= Voltage on CALO (Minimum Voltage 450V)\\ | ||
+ | Ebeam = Energy beam [MeV]\\ | ||
+ | E0 = 447 [MeV]\\ | ||
+ | \\ | ||
+ | |||
+ | **TABLE @ 447 MeV**\\ | ||
+ | **Last calibration @450MeV 20220505**\\ | ||
+ | |||
+ | ^ V ^ N ^ lastcal N m=1 ^ sigma lastcal | ||
+ | | 1300 | 360.9 | 350.6 | 41.8 | | ||
+ | | 1200 | 186.75 | ||
+ | | 1100 | 92.51 | 96.1 | 11,4 | | ||
+ | | 1000 | 42.54 | 45.3 | 5.6 | | ||
+ | | 900 | 18.03 | 19.6 | 2.58 | | ||
+ | | 800 | 6.903 | 8.23 || | ||
+ | | 700 | 2.325 | 2.78 || | ||
+ | | 600 | 0.662 | 0.84 || | ||
+ | | 500 | 0.1507 | ||
+ | | 450 || 0.092 || | ||
+ | | 400 | ||
+ | |||
+ | |||
+ | **Oscilloscope to Multiplicity calibration**\\ | ||
+ | To recover multiplicity by your own measurement system with our CALOBTF1 signal, follow these steps:\\ | ||
+ | * Usually we will refer our measurement with our QDC Caen V965 (old Type, 800[pC] full scale in 12bit, output is in ADC values) | ||
+ | * acquire the signal in time domain | ||
+ | * give an integration time about 200[ns], centred on Beam signal (typically CALOBTF1 signal Tr=8[ns], Tf=20[ns]) to pick up best baseline | ||
+ | * measure integrate pedestal without beam signal (P). Oscilloscope will give you values in [V*s], to get value in [pC], divide by your input impedance. | ||
+ | * measure the integrated gate signal (GS) and removing pedestal value and get your signal (S) then [mV*ns/ | ||
+ | * Multiplicity (M) is this value normalized in our ADC scale value, divided by N , single particle value (see table on top for CALOBTF1, voltage and beam energy dependant) | ||
+ | |||
+ | S=(GS-P)/ | ||
+ | M=S/ | ||
+ | \\ | ||
+ | **CALO as BACKGROUND gamma detector for HIGH INTENSITY operation on N@BTF**\\ | ||
+ | We can use CALOBTF1 as background gamma detector to discover the upper limit of gamma to prevent the safety sistem to trips.\\ | ||
+ | We put CALOBTF1 in the bent middle line at 3.8 meters from exit bent pipe with 500V supply\\ | ||
+ | Normal operation means up to 20mV peak to peak signal, if above the safety trips\\ | ||
+ |
strutture/lnf/da/btf/dispositivi/rivelatori/calorimeter/cherenkov.txt · Last modified: 2022/12/21 16:19 by foggetta@infn.it