Abstract

We have measured the $\gamma$-ray energy spectrum from the thermal neutron capture, ${}^{157}$Gd$(n,\gamma){}^{158}$Gd, on an enriched $^{157}$Gd target (Gd$_{2}$O$_{3}$) in the energy range from 0.11 MeV up to about 8 MeV. The target was placed inside the germanium spectrometer of the ANNRI detector at J-PARC and exposed to a neutron beam from the Japan Spallation Neutron Source (JSNS). Radioactive sources ($^{60}$Co, $^{137}$Cs, and $^{152}$Eu) and the reaction $^{35}$Cl($n$,$\gamma$) were used to determine the spectrometer's detection efficiency for $\gamma$ rays at energies from 0.3 to 8.5 MeV. Using a Geant4-based Monte Carlo simulation of the detector and based on our data, we have developed a model to describe the $\gamma$-ray spectrum from the thermal ${}^{157}$Gd($n$,$\gamma$) reaction. While we include the strength information of 15 prominent peaks above 5 MeV and associated peaks below 1.6 MeV from our data directly into the model, we rely on the theoretical inputs of nuclear level density and the photon strength function of ${}^{158}$Gd to describe the continuum $\gamma$-ray spectrum from the ${}^{157}$Gd($n$,$\gamma$) reaction. Our model combines these two components. The results of the comparison between the observed $\gamma$-ray spectra from the reaction and the model are reported in detail.

Highlights

  • Gadolinium, 6A4Gd, is a rare earth element

  • A good model for the γ -ray energy spectrum from the radiative thermal neutron capture on natural gadolinium is an important prerequisite for Monte Carlo (MC) studies to evaluate the efficiency of tagging neutrons from inverse beta decay (IBD) events in gadolinium-enhanced νe searches

  • Using the Ge spectrometer of the Accurate Neutron–Nucleus Reaction Measurement Instrument (ANNRI) detector at MLF, J-PARC, we performed a measurement of the γ -ray energy spectrum from thermal neutron capture on 157Gd

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Summary

Introduction

Gadolinium, 6A4Gd, is a rare earth element. Its natural composition (natGd) includes isotopes with the atomic mass numbers A = 152, 154–158, and 160. It has become a common technique to add a mass fraction of 0.1–0.2% of gadolinium into the neutrino targets of organic liquid scintillator [15,16,17] and water Cherenkov [19,20,38,39] detectors in order to enhance the neutron tagging efficiency for IBD events. Good understanding of the multiplicities of γ rays from Gd(n, γ ) reactions and their energy distributions in the range 0.1–8 MeV is an important prerequisite to proper prediction of neutron tagging efficiencies in gadolinium-loaded water Cherenkov detectors based on MC simulations. Background and calibration data In order to measure the background for the experiment, which originates mostly from γ rays from the interactions of the beam neutrons with materials other than the target, we placed the empty target

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