1992
DOI: 10.1016/0168-9002(92)90209-m
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Experimental investigation of statistical models describing distribution of counts

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Cited by 7 publications
(3 citation statements)
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“…The electron emission is then inhomogeneous Poisson process and the variation of the expected number of initiating electrons k λ with time t can be described by k λ = ke ±λt (where λ is the increase/decrease rate and k is the expected value of initiating electrons in the stationary case), as in refs. [27][28][29]. When the time variations are slow, it can be approximated by which is analogous to the electron yield variation in ref.…”
Section: Electron Avalanche Number Distributions When the Electron Em...mentioning
confidence: 99%
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“…The electron emission is then inhomogeneous Poisson process and the variation of the expected number of initiating electrons k λ with time t can be described by k λ = ke ±λt (where λ is the increase/decrease rate and k is the expected value of initiating electrons in the stationary case), as in refs. [27][28][29]. When the time variations are slow, it can be approximated by which is analogous to the electron yield variation in ref.…”
Section: Electron Avalanche Number Distributions When the Electron Em...mentioning
confidence: 99%
“…where the distribution weighting factors Besides that, this model can describe the electron number distributions for electron avalanches initiated by short lived radionuclides [27][28][29]32]. Also, it can be applied to electron avalanches in accelerated aging tests [26] and with aging effects correlated to construction materials, surface processes, operational gas gain, gas mixtures and flow rates, gas impurities, etc.…”
Section: Electron Avalanche Number Distributions When the Electron Em...mentioning
confidence: 99%
“…Equations ( 28) and ( 29) are generalizations of equations (11) and (10), respectively. Together with equation ( 25) they reproduce the statistics of a 30% spectral fraction seen in figure 4.…”
Section: Dispersion With Pileup and Edtmentioning
confidence: 99%