Difference between revisions of "2NCorr SPDP Introduction"
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[[Production Analysis | go_back ]] | [[Production Analysis | go_back ]] | ||
| − | Our array of detectors has a highly non-uniform neutron efficiency and acceptance w.r.t. neutron-neutron opening angle. This is due to the array's non-spherically symmetric geometry, and to its neutron detection efficiency as a function of both particle position and energy (see figure). For this reason, every measured distribution | + | Our array of detectors has a highly non-uniform neutron efficiency and acceptance w.r.t. neutron-neutron opening angle (<math>#theta_{n-n}</math>). This is due to the array's non-spherically symmetric geometry, and to its neutron detection efficiency as a function of both particle position and energy (see figure). For this reason, every measured distribution is made meaningful by the normalizing against another distribution. For <math>#theta_{n-n}</math> |
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| + | [[File:2N Corr OpeningAngleCf252.png|thumb| right|400px| Measured opening angle distribution of uncorrelated neutrons from Cf252 target.]] | ||
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Revision as of 21:46, 19 January 2018
Our array of detectors has a highly non-uniform neutron efficiency and acceptance w.r.t. neutron-neutron opening angle (). This is due to the array's non-spherically symmetric geometry, and to its neutron detection efficiency as a function of both particle position and energy (see figure). For this reason, every measured distribution is made meaningful by the normalizing against another distribution. For
