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Uncertainties analysis of fission fraction for reactor antineutrino experiments

2014/05/27 by X. B. Ma, X. B., Ma, X. B. +13 · 1 citation
Physics and Astronomy · #Astrophysics and Cosmic Phenomena #FOS: Physical sciences #Instrumentation and Detectors (physics.ins-det) #Neutrino Physics Research #Nuclear Experiment (nucl-ex) #Particle physics theoretical and experimental studies #nucl-ex #physics.ins-det

paper · pdf · doi:10.48550/arxiv.1405.6807

arXiv admin note: substantial text overlap with arXiv:1109.5379, arXiv:1101.2266 by other authors

openalex publication_date 2014/05/27 · arxiv created 2015/03/17 · arxiv updated 2015/03/18 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28

Abstract

Reactor antineutrino experiment are used to study neutrino oscillation, search for signatures of nonstandard neutrino interaction, and monitor reactor operation for safeguard application. Reactor simulation is an important source of uncertainties for a reactor neutrino experiment. Commercial code is used for reactor simulation to evaluate fission fraction in Daya Bay neutrino experiment, but the source code doesn't open to our researcher results from commercial secret. In this study, The open source code DRAGON was improved to calculate the fission rates of the four most important isotopes in fissions, 235U,238U,239Pu and 241Pu, and then was validated for PWRs using the Takahama-3 benchmark. The fission fraction results are consistent with those of MIT's results. Then, fission fraction of Daya Bay reactor core was calculated by using improved DRAGON code, and the fission fraction calculated by DRAGON agreed well with these calculated by SCIENCE. The average deviation less than 5% for all the four isotopes. The correlation coefficient matrix between 235U,238U,239Pu and 241Pu were also studied using DRAGON, and then the uncertainty of the antineutrino flux by the fission fraction was calculated by using the correlation coefficient matrix. The uncertainty of the antineutrino flux by the fission fraction simulation is 0.6% per core for Daya Bay antineutrino experiment. The uncertainties source of fission fraction calculation need further to be studied in the future.

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