2002
DOI: 10.1016/s0168-9002(01)01623-0
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On the physical origin of tails in the time response of spark counters

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Cited by 44 publications
(17 citation statements)
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“…A simple theory of the RPC timing properties may be formulated on the following principles (see also [6], [7], [8]). The poissonian probability that k>0 clusters will be produced in the sensitive region of the gap from the N * average effective clusters is given by *…”
Section: Timing Resolutionmentioning
confidence: 99%
See 1 more Smart Citation
“…A simple theory of the RPC timing properties may be formulated on the following principles (see also [6], [7], [8]). The poissonian probability that k>0 clusters will be produced in the sensitive region of the gap from the N * average effective clusters is given by *…”
Section: Timing Resolutionmentioning
confidence: 99%
“…1 Calculations suggest that the detailed form of the avalanche gain statistics has a negligible influence on the time resolution ( [6], [8]), being reasonable to consider the simplest case.…”
Section: Timing Resolutionmentioning
confidence: 99%
“…In such a high electric field, the process, once started, goes on until practically all gas in the cell is ionized; an uncontrolled discharge can be prevented by restricting the electric field by space charge effects and/or by external means, e.g., a resistor in the HV bias chain, as in the Geiger counter. In our design, the discharge stops when the voltage across the cell drops due to the high-volume resistivity of the cathode; this is similar to the limited streamer process occurring, e.g., in Resistive Plate Chambers (RPC) [5]. The discharge is restricted not only in time but in space, as it remains confined to the cell where it started.…”
Section: Detector Operational Principle and Designmentioning
confidence: 87%
“…This can be understood when looking at Fig. 11a and it is a well-established fact for detectors like Resistive Plate Chambers [13], where avalanche fluctuations dominate the signal characteristics [14,15]: scaling the threshold by a constant c 1 will just shift the time response function by ∆t = (ln c 1 )/λ t without altering its shape. If we are not interested in the absolute time of the threshold crossing but just the time variations we can arbitrarily set n = 1 and have the time response function…”
Section: Avalanches In Absence Of Boundariesmentioning
confidence: 88%