JOURNAL ARTICLE
Cross-sections for nuclear transmutation of long-lived fission product 126Sn using (p,n) reaction.
Published In: International Journal of Modern Physics E: Nuclear Physics, 2024, v. 33, n. 1/2. P. 1 1 of 3
Database: Academic Search Ultimate 2 of 3
Authored By: Churi, K.; Singh, P.; Hinge, S.; Hemalatha, M. 3 of 3
Abstract
For a sustainable nuclear energy program using fission reactors, the reduction or elimination of long-lived radioactive waste is essential. The hazardous Long-Lived Fission Products (LLFP), which are by-products of the operation of nuclear reactors, need to be converted to short-lived or stable nuclei. For nuclear transmutation, the knowledge of reaction cross-sections is important. The cross-section and half-life for the proton-induced transmutation of the LLFP, 1 2 6 Sn, produced as nuclear waste from the reactor have been calculated. The cross-section for the (p,n) reaction on unstable 1 2 6 Sn has been calculated using phenomenological as well as microscopic models of optical potentials and level densities in the framework of the statistical nuclear model using the latest version of the code TALYS-1.96. The Koning–Delaroche (KD) and Jeukenne–Lejeune–Mahaux–Bruyeres (JLMB) optical models, as well as back-shifted Fermi gas model (BFM) and Hartree–Fock (HF) level density, based on the Skyrme force from Gorielys tables, have been used. The renormalized optical model parameters and level density models obtained by comparing cross-sections with data for protons incident on stable 1 1 2 , 1 1 4 , 1 1 5 , 1 1 6 , 1 1 7 , 1 1 8 , 1 1 9 , 1 2 0 , 1 2 2 , 1 2 4 Sn isotopes were extended to make a prediction of (p,n) cross-section on unstable 1 2 6 Sn isotope. The excitation function obtained using JLMB-HF calculation for 1 2 6 Sn reveals a peak at an incident proton energy of 8.5 MeV with a corresponding cross-section of 269 mb. It would be of interest to perform experiments for measurements of cross-section where data are unavailable, especially in the peak regions and beyond, to validate the predictions of this work. It is found that for a proton flux of 6. 2 5 × 1 0 1 4 s − 1 cm − 2 , and a peak cross-section calculated using JLMB-HF calculation, the effective half-life of transmutation of 1 2 6 Sn is about 65 years, thus justifying its feasibility. [ABSTRACT FROM AUTHOR]
Additional Information
- Source:International Journal of Modern Physics E: Nuclear Physics. 2024/01, Vol. 33, Issue 1/2, p1
- Document Type:Article
- Subject Area:Physics
- Publication Date:2024
- ISSN:0218-3013
- DOI:10.1142/S021830132450006X
- Accession Number:176278169
- Copyright Statement:Copyright of International Journal of Modern Physics E: Nuclear Physics is the property of World Scientific Publishing Company and its content may not be copied or emailed to multiple sites without the copyright holder's express written permission. Additionally, content may not be used with any artificial intelligence tools or machine learning technologies. However, users may print, download, or email articles for individual use. This abstract may be abridged. No warranty is given about the accuracy of the copy. Users should refer to the original published version of the material for the full abstract. (Copyright applies to all Abstracts.)
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