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    Inelastic neutron scattering on U238 with γ-ray coincidence spectroscopy

    Carole Chatel1,2,3,4,*,†, Jonathan Wilson5, Philippe Dessagne1, Greg Henning1, Maëlle Kerveno1, P. Aguilera6,7,8, A. Algora9,10, G. de Angelis11, J. Benito6,7,12 et al. (Nu-Ball Collaboration)

    J. Benito6,7,12, D. Bittner13, A. Blazhev13, S. Bottoni14,15, J. A. Briz16, R. Canavan17,18, F. Didierjean1, G. Duchêne1, A. Esmaylzadeh13, J. Fischer13, B. Fornal19, L. M. Fraile16, E. R. Gamba14,15, R. B. Gerst13, K. A. Gladnishki20, G. Häfner5,13, K. Hauschild5, J. Heery17, C. Henrich2, C. Hiver5, I. Homm2, Ł. W. Iskra19, N. Jovancevic21, D. Kalaydjieva22, L. Knafla13, D. Knezevic23, D. Kocheva20, A. Korgul24, G. Kosir25,26, T. Kröll2,4, M. Lebois5, S. Leoni14,15, J. Ljungvall1,5, M. Llanos-Expósito16, A. Lopez-Martens5, E. Lovšin25,26, R. Lozeva5, M. Markova27, A. Messingschlager2, K. Miernik24, T. Milanovic28, M. Moukaddam1, J. R. Murias16,29, A. Oberstedt30, S. Oberstedt31, S. Pascu17,32, G. Pasqualato5, W. Paulsen27, Zs. Podolyák17, W. Poklepa7,24, P. H. Regan17,18, K. Rezynkina6, M. Rudigier2,4, V. Sánchez-Tembleque16, K. Solak24, K. Stoychev33, M. Stryjczyk34,35, C. Sürder2,4, D. Thisse22, Ma. von Tresckow2,4, V. Vedia16,36, J. Vesic25, and N. Warr13 (Nu-Ball Collaboration)

    • 1Université de Strasbourg, CNRS, IPHC/DRS UMR 7178, 23 Rue du Loess, F-67037 Strasbourg, France
    • 2Technische Universität Darmstadt, Fachbereich Physik, Institut für Kernphysik, Schlossgartenstrasse, 9, 64289 Darmstadt, Germany
    • 3GSI Helmholtzzentrum für Schwerionenforschung, 64291 Darmstadt, Germany
    • 4Helmholtz Research Academy Hesse for FAIR (HFHF), GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
    • 5CNRS, IJClab Orsay, bât 100, 15 rue G. Clemenceau, 91406 Orsay Cedex, France
    • 6Istituto Nazionale di Fisica Nucleare, Sezione di Padova, Padova, Italy
    • 7Università degli Studi di Padova, Padova, Italy
    • 8Centro de Investigación en Física Nuclear y Espectroscopia de Neutrones CEFNEN, Comisión Chilena de Energía Nuclear, Santiago, Chile
    • 9IFIC, CSIC-University of Valencia, Valencia, Spain
    • 10HUN-REN Institute of Nuclear Research, Debrecen, Hungary
    • 11INFN Laboratori Nazionali di Legnaro, Legnaro, Italy
    • 12Grupo de Fisica Nuclear, Universidad Complutense de Madrid, Madrid, Spain
    • 13Institut für Kernphysik, Universität zu Köln, Cologne, Germany
    • 14Dipartimento di Fisica, Universitá degli Studi di Milano, Milan, Italy
    • 15Istituto Nazionale di Fisica Nucleare sez. Milano, Milan, Italy
    • 16Grupo de Física Nuclear, EMFTEL & IPARCOS, Universidad Complutense de Madrid, CEI Moncloa, E-28040 Madrid, Spain
    • 17School of Mathematics. Physics and Space, University of Surrey, Guildford GU2 7XH, United Kingdom
    • 18Medical Marine and Nuclear Department, National Physical Laboratory, Teddington TW11 0LW, United Kingdom
    • 19Institute of Nuclear Physics, Polish Academy of Sciences, Krakow, Poland
    • 20Faculty of Physics, St. Kliment Ohridski University of Sofia, 1164 Sofia, Bulgaria
    • 21University of Novi Sad, Novi Sad, Serbia
    • 22IRFU/DPhN, CEA Saclay, Université Paris-Saclay, 91191 Gif-sur-Yvette, France
    • 23Institute of Physics Belgrade, Belgrade, Serbia
    • 24Faculty of Physics, University of Warsaw, PL 02-093 Warsaw, Poland
    • 25Jožef Stefan Institute, Ljubljana, Slovenia
    • 26University of Ljubljana, Ljubljana, Slovenia
    • 27Department of Physics, University of Oslo, Oslo, Norway
    • 28Vinča Institute of Nuclear Sciences, Belgrade, Serbia
    • 29Rutherford Appleton Laboratory - UKRI, Didcot OX11 0QX, United Kingdom
    • 30Extreme Light Infrastructure - Nuclear Physics, “Horia Hulubei” National Institute for R&D in Physics and Nuclear Engineering, 30 Reactorului Street, 077125 Magurele, Romania
    • 31European Commission, Joint Research Centre, Directorate for Nuclear Safety and Security, 2440 Geel, Belgium
    • 32“Horia Hulubei” National Institute for R&D in Physics and Nuclear Engineering, R-77125 Bucharest-Magurele, Romania
    • 33Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France
    • 34University of Jyvaskyla, Department of Physics, Accelerator Laboratory, P.O. Box 35(YFL) FI-40014 University of Jyvaskyla, Finland
    • 35Institut Laue-Langevin, 71 Avenue des Martyrs, F-38042 Grenoble, France
    • 36ISOLDE, CERN, 1211 Geneva 23, Switzerland

    • *Contact author: carole.chatel@eli-np.ro
    • †Present address: Extreme Light Infrastructure - Nuclear Physics, IFIN-HH, 30 Reactorului Street, 077125 Magurele, Romania.

    Phys. Rev. C 113, 064320 – Published 30 June, 2026

    DOI: https://doi.org/10.1103/jrh6-rh6h

    Abstract

    Improvement of the accuracy of neutronics simulation of actual or future reactor designs is essential and requires a better knowledge of the core neutron population. The reactor neutron population is partially driven by (n,xn) reactions that change the number and decrease the energy of the neutrons. However, the cross sections of these reactions are currently not measured with sufficient precision. This is particularly the case for the neutron inelastic-scattering cross section of U238, which represents around 90%–95% of the mass of fuel in present and many future reactor core designs. It therefore features on the High Priority Request List for measurement improvement. This cross section can be measured using prompt γ-ray spectroscopy coupled to neutron time-of-flight measurements, where the total (n,n′) cross section can be deduced from a combination of the measured (n,n′γ) partial cross sections and the level scheme information. The knowledge of the U238 level scheme is still very incomplete, inducing significant uncertainties on the resulting inelastic-scattering cross section. Therefore, an effort has recently been carried out to experimentally revisit the U238 decay scheme by performing high-resolution coincidence spectroscopy of the U238(n,n′) reaction. To obtain detailed level scheme information, the ν-Ball γ spectrometer was coupled to the LICORNE directional neutron source of the ALTO facility, allowing the study of inelastic scattering of fast neutrons (0.5–3 MeV) on U238 via γ−γ coincidence spectroscopy. Coincidence matrices obtained during the first and the second ν-Ball campaigns were analyzed using the RadWare ESCL8R software. 110 γ transitions and 60 levels registered in the Evaluated Nuclear Structure Data File database have been confirmed, and 158 new γ transitions and 58 new levels have been found. Although not exhaustive, the U238 level scheme information has been significantly improved, and its completeness has been estimated to be up to 1.7214 MeV compared with 1.27854 MeV at present. It is hence expected to decrease the uncertainties of U238 (n,n′) cross sections, which is needed for accurate reactor core modeling.

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    Corrections

    22 July, 2026

    Correction: An incorrect affiliation indicator for author T. Kröll has been fixed.

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