Abstract

The neutron-capture reaction produces a large variety of γ-ray cascades with different γ-ray multiplicities. A measured spectral distribution of these cascades for each γ-ray multiplicity is of importance to applications and studies of γ-ray statistical properties. The DANCE array, a 4π ball of 160 BaF2 detectors, is an ideal tool for measurement of neutron-capture γ-rays. The high granularity of DANCE enables measurements of high-multiplicity γ-ray cascades. The measured two-dimensional spectra (γ-ray energy, γ-ray multiplicity) have to be corrected for the DANCE detector response in order to compare them with predictions of the statistical model or use them in applications. The detector-response correction problem becomes more difficult for a 4π detection system than for a single detector. A trial and error approach and an iterative decomposition of γ-ray multiplets, have been successfully applied to the detector-response correction. Applications of the decomposition methods are discussed for two-dimensional γ-ray spectra measured at DANCE from γ-ray sources and from the 10B(n, γ) and 113Cd(n, γ) reactions.

Highlights

  • The (n, γ) resonances de-excite via γ-ray cascades with various multiplicities

  • Applications of the decomposition methods are discussed for two-dimensional γ-ray spectra measured at Detector for Advanced Neutron Capture Experiments (DANCE) from γ-ray sources and from the 10 B(n, γ) and 113 Cd(n, γ) reactions

  • The Detector for Advanced Neutron Capture Experiments (DANCE) is an excellent tool to measure the spectra from the (n, γ) resonances because of its high granularity, high efficiency and near 4π coverage

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Summary

Introduction

The (n, γ) resonances de-excite via γ-ray cascades with various multiplicities. The γ-ray spectra for each γ-ray multiplicity (Mγ ) have different intensity distributions (Iγ )characteristic for the product nucleus from the reaction and the (n, γ) resonance. Applications of the decomposition methods are discussed for two-dimensional γ-ray spectra measured at DANCE from γ-ray sources and from the 10 B(n, γ) and 113 Cd(n, γ) reactions. The spectra have to be corrected for the detector response in order to obtain the γ-ray intensities emitted by the target.

Results
Conclusion

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