Abstract

In the normal operation of nuclear reactors, the kinetic behavior of the neutron population in the core is driven by the so-called delayed neutrons (DN). The DN yield per fission, their average lifetime and their groups’ abundances are the main physical parameters used to predict the kinetic behavior of the reactor and its reactivity. The overall uncertainty associated to reactivity predictions, which is linked directly to the nuclear reactor safety margins, is thus closely dependent on a few parameters associated with DN. Depending on the nuclear data library, DN kinetic parameters present significant discrepancies, even for major fissile isotopes such as 235U or 239Pu. In this context, CEA has long been working for improving DN nuclear data. In 2018, CEA launched the ALDEN project (Average Lifetime of DElayed Neutrons) in the framework of a collaboration between CEA/DES, CEA/DRF, CNRS/IN2P3 (LPSC, CENBG, LPC), ENSICAEN and Caen University. This program aims at measuring the kinetics of the delayed neutrons to derive the DN yield, their average lifetime and abundances. Two experimental campaigns focusing on the thermal fission of 235U were conducted in 2018 and 2019. They demonstrated the concept feasibility and gave high quality estimations of the DN multiplicity (1.631 ± 0.014 %) and average lifetime (8.82 ± 0.6 s) for 235U. More recently in March 2021, a more ambitious irradiation campaign was conducted on 239Pu and 233U. This paper details the new experimental setup, which was upgraded to meet ILL safety requirements for handling plutonium. The data analysis process is presented, with a focus on the problem of dead time correction. Finally, some preliminary delayed neutron decay curves are showed and discussed.

Highlights

  • IN nuclear reactor physics, some fission products are referred to as “delayed neutron precursors” because they undergo a ( +n) radioactive decay and produce neutrons long after the fission

  • In a thermal fission nuclear reactor, the delayed neutrons (DN) population is roughly 0.7 % of the total number of neutrons, but it still drives the kinetic behavior of the nuclear reactor

  • In nuclear data libraries, such as ENDF-B/VII or JEFF3.1.1, inconsistencies on some major parameters describing DN precursors can still be found [1]. This is especially true for the average lifetime of DN precursors, as well as for the average number of DN per fission

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Summary

Introduction

IN nuclear reactor physics, some fission products are referred to as “delayed neutron precursors” because they undergo a ( +n) radioactive decay and produce neutrons long after the fission (from milliseconds to several minutes). In nuclear data libraries, such as ENDF-B/VII or JEFF3.1.1, inconsistencies on some major parameters describing DN precursors can still be found [1]. This is especially true for the average lifetime of DN precursors, as well as for the average number of DN per fission ( called DN multiplicity or DN yield). In this context, CEA has long been working on improving nuclear data evaluation of DN precursors. This is the reason why a new experiment was designed with the aim of studying the thermal fission of several actinides of interest, among them: 235U, 239Pu, 233U and 241Pu

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