Difference between revisions of "Theoretical analysis of 2n accidentals rates"
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Revision as of 03:31, 20 January 2018
Introduction
A given photon pulse may cause multiple neutron-producing reactions, ranging from zero to "infinity" reactions. The number of neutron-producing reactions in a pulse is hereafter denoted by
. Being the number of neutron-producing reactions actually occurring per pulse, is assumed to follow the Poissonian distribution as a limiting case of the binomial distribution. Each neutron-producing interaction is said to produce correlated neutrons, where the random variable is the distribution of the number of neutrons produced in a single neutron-producing reaction. Each of the are independent and identically distributed random variables, so the purpose of the subscript is to distinguish between several distinct neutron-producing interactions which may occur in a single pulse.The beam has a Bremsstrahlung end point of 10.5 MeV, which energetically allows for only two possible neutron-producing interactions, 1n-knochout and photofission. Thus,
is equal to the photofission neutron multiplicity plus a contribution at from 1n-knockout events. The analysis that follows does not need to distinguish between 1n-knockout events and photofission events that emit a single neutron. In both cases, a single neutron is emitted and is uncorrelated with all and any other neutrons.Variable reference
Variable | Description |
---|---|
A random variable for the number of neutron producing reactions occurring in a single pulse. | |
A random variable for the number of correlated neutrons produced by the | neutron-producing reaction in a given pulse. The index , ranging from 1 to , is used to distinguish between each of the distinct and independent reactions in a given pulse, thus all the are identical and independently distributed random variables
Probability of detecting an accidental from a given pulse
note1
test