2015
DOI: 10.1016/j.nima.2014.11.065
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Performance investigation of the pulse and Campbelling modes of a fission chamber using a Poisson pulse train simulation code

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Cited by 33 publications
(19 citation statements)
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“…In order to systematize and unify these observations, a well-known reference model for intermittent fluctuations [30][31][32][33][34][35][36][37] has been introduced for SOL plasma fluctuations [38][39][40]. This model, called a shot noise process or filtered Poisson process (FPP), consists of a super-position of independent and identical pulse shapes with randomly distributed amplitudes, arriving according to a Poisson process.…”
mentioning
confidence: 99%
“…In order to systematize and unify these observations, a well-known reference model for intermittent fluctuations [30][31][32][33][34][35][36][37] has been introduced for SOL plasma fluctuations [38][39][40]. This model, called a shot noise process or filtered Poisson process (FPP), consists of a super-position of independent and identical pulse shapes with randomly distributed amplitudes, arriving according to a Poisson process.…”
mentioning
confidence: 99%
“…There is still room for improvement, the COSICAF database is still reduced but additional materials and heavy ions could be easily integrated. Campbell and current mode could also be simulated from the computed pulses with additional work [1], [21]. Even if the software assumes strong approximations, it was shown that for fission chamber signal, the quantitative results are in rather good agreement with the experimental ones.…”
Section: Discussionmentioning
confidence: 99%
“…Depending on the neutron flux and the ionisation chamber design, it is possible to operate such detector in three different modes [1]: pulse mode where pulses doesn't overlap; Campbell mode where pulses pile up but it is possible to link the count rate to signal variance; current mode, where the signal is high enough to produce a current proportional to the count rate [2].…”
Section: Introductionmentioning
confidence: 99%
“…This reaction results in two high energy fission fragments (FF), around 166 MeV in total [10], which subsequently are emitted in opposite directions. One FF passes through the gas, whereas the other one is absorbed by the anode [11].…”
Section: Fission Chambers (Fc)mentioning
confidence: 99%