Difference between revisions of "Some specifications on PMTs"
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''' Pulse amplitude''' | ''' Pulse amplitude''' | ||
− | * Assume a triangular pulse | + | * Assume a triangular pulse 20 ns wide |
− | * Umax = ( 2 / | + | * Umax = ( 2 / 20 ns ) x Np.e. x Gain x 1.6 10^-19 x 50 Om = '''64 mV''' |
− | * | + | * 128 mV for operating at two times smaller rate of 2 MHz (i.e., two times higher gain) |
− | + | * The signal pulse has to be splitted (FADC250 and LE/F1TDC) | |
* We should consider to use amplifiers | * We should consider to use amplifiers |
Latest revision as of 09:54, 21 September 2012
Light yield estimates
- 5 mm thick scintillators
- 10000 initial photons per tagged electron
- assume that 2000 photons are collected (20 % light collection efficiency)
- 400 p.e. (assuming 20% quantum efficiency)
Counter rates (according to the latest Dan's design)
- 1.1 μ A electron current, radiator
- (corresponds to the photon flux of phot/sec in the cohrent peak region)
- Counter rate around E_gamma = 9 GeV: 1 - 1.5 MHz
- (counter with ~20 MeV)
- The rate is about 4 times larger for the last counter (at 3 GeV)
Operating gain
- Assume 4 MHz counter rate, 400 p.e., 50 μA anode current
- The maximum anode current is typically 100 μ A. We have to operate tubes at at least 2 times smaller current.
- Gain = A / (Rate x Np.e. x 1.6 10^-19) =
Pulse amplitude
- Assume a triangular pulse 20 ns wide
- Umax = ( 2 / 20 ns ) x Np.e. x Gain x 1.6 10^-19 x 50 Om = 64 mV
- 128 mV for operating at two times smaller rate of 2 MHz (i.e., two times higher gain)
- The signal pulse has to be splitted (FADC250 and LE/F1TDC)
- We should consider to use amplifiers