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Measurement of the <math><mrow><mmultiscripts><mi mathvariant='normal'>N</mi><mprescripts/><none/><mn>14</mn></mmultiscripts><mo>(</mo><mi>n</mi><mo>,</mo><mi>p</mi><mo>)</mo><mmultiscripts><mi mathvariant='normal'>C</mi><mprescripts/><none/><mn>14</mn></mmultiscripts></mrow></math> cross section at the CERN n_TOF facility from subthermal energy to 800 keV

Authors :
Torres-Sánchez, Pablo
Praena, Javier
Porras, Ignacio
Sabaté-Gilarte, Marta
Lederer-Woods, Claudia
Aberle, Oliver
Alcayne, Victor
Amaducci, Simone
Andrzejewski, Józef
Audouin, Laurent
Bécares, Vicente
Babiano-Suarez, Victor
Bacak, Michael
Barbagallo, Massimo
Bečvář, František
Bellia, Giorgio
Berthoumieux, Eric
Billowes, Jon
Bosnar, Damir
Brown, Adam
Busso, Maurizio
Caamaño, Manuel
Caballero, Luis
Calviño, Francisco
Calviani, Marco
Cano-Ott, Daniel
Casanovas, Adria
Cerutti, Francesco
Chen, Yonghao
Chiaveri, Enrico
Colonna, Nicola
Cortés, Guillem
Cortés-Giraldo, Miguel
Cosentino, Luigi
Cristallo, Sergio
Damone, Lucia-Anna
Diakaki, Maria
Dietz, Mirco
Domingo-Pardo, César
Dressler, Rugard
Dupont, Emmeric
Durán, Ignacio
Eleme, Zinovia
Fernández-Domínguez, Beatriz
Ferrari, Alfredo
Ferrer, Francisco Javier
Finocchiaro, Paolo
Furman, Valter
Göbel, Kathrin
Garg, Ruchi
Gawlik-Ramięga, Aleksandra
Geslot, Benoit
Gilardoni, Simone
Glodariu, Tudor
Gonçalves, Isabel
González-Romero, Enrique
Guerrero, Carlos
Gunsing, Frank
Harada, Hideo
Heinitz, Stephan
Heyse, Jan
Jenkins, David
Jericha, Erwin
Käppeler, Franz
Kadi, Yacine
Kimura, Atsushi
Kivel, Niko
Kokkoris, Michael
Kopatch, Yury
Krtička, Milan
Kurtulgil, Deniz
Ladarescu, Ion
Leeb, Helmut
Lerendegui-Marco, Jorge
Meo, Sergio Lo
Lonsdale, Sarah-Jane
Macina, Daniela
Manna, Alice
Martínez, Trinitario
Masi, Alessandro
Massimi, Cristian
Mastinu, Pierfrancesco
Mastromarco, Mario
Matteucci, Francesca
Maugeri, Emilio-Andrea
Mazzone, Annamaria
Mendoza, Emilio
Mengoni, Alberto
Michalopoulou, Veatriki
Milazzo, Paolo Maria
Mingrone, Federica
Musumarra, Agatino
Negret, Alexandru
Nolte, Ralf
Ogállar, Francisco
Oprea, Andreea
Patronis, Nikolas
Pavlik, Andreas
Perkowski, Jarosław
Persanti, Luciano
Quesada, José-Manuel
Radeck, Désirée
Ramos-Doval, Diego
Rauscher, Thomas
Reifarth, René
Rochman, Dimitri
Rubbia, Carlo
Saxena, Alok
Schillebeeckx, Peter
Schumann, Dorothea
Smith, Gavin
Sosnin, Nikolay
Stamatopoulos, Athanasios
Tagliente, Giuseppe
Tain, José
Talip, Zeynep
Tarifeño-Saldivia, Ariel
Tassan-Got, Laurent
Tsinganis, Andrea
Ulrich, Jiri
Urlass, Sebastian
Valenta, Stanislav
Vannini, Gianni
Variale, Vincenzo
Vaz, Pedro
Ventura, Alberto
Vlachoudis, Vasilis
Vlastou, Rosa
Wallner, Anton
Woods, Philip John
Wright, Tobias
Žugec, Petar
Institut de Physique Nucléaire d'Orsay (IPNO)
Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)
Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU)
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay
CEA Cadarache
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)
n_TOF
Source :
Phys.Rev.C, Phys.Rev.C, 2023, 107 (6), pp.064617. ⟨10.1103/PhysRevC.107.064617⟩
Publication Year :
2023
Publisher :
HAL CCSD, 2023.

Abstract

International audience; Background: The N14(n,p)C14 reaction is of interest in neutron capture therapy, where nitrogen-related dose is the main component due to low-energy neutrons, and in astrophysics, where N14 acts as a neutron poison in the s process. Several discrepancies remain between the existing data obtained in partial energy ranges: thermal energy, keV region, and resonance region.Purpose: We aim to measure the N14(n,p)C14 cross section from thermal to the resonance region in a single measurement for the first time, including characterization of the first resonances, and provide calculations of Maxwellian averaged cross sections (MACS).Method: We apply the time-of-flight technique at Experimental Area 2 (EAR-2) of the neutron time-of-flight (n_TOF) facility at CERN. B10(n,α)Li7 and U235(n,f) reactions are used as references. Two detection systems are run simultaneously, one on beam and another off beam. Resonances are described with the R-matrix code sammy.Results: The cross section was measured from subthermal energy to 800 keV, resolving the first two resonances (at 492.7 and 644 keV). A thermal cross section was obtained (1.809&#177;0.045 b) that is lower than the two most recent measurements by slightly more than one standard deviation, but in line with the ENDF/B-VIII.0 and JEFF-3.3 evaluations. A 1/v energy dependence of the cross section was confirmed up to tens of keV neutron energy. The low energy tail of the first resonance at 492.7 keV is lower than suggested by evaluated values, while the overall resonance strength agrees with evaluations.Conclusions: Our measurement has allowed determination of the N14(n,p) cross section over a wide energy range for the first time. We have obtained cross sections with high accuracy (2.5%) from subthermal energy to 800 keV and used these data to calculate the MACS for kT=5 to kT=100 keV.

Details

Language :
English
Database :
OpenAIRE
Journal :
Phys.Rev.C, Phys.Rev.C, 2023, 107 (6), pp.064617. ⟨10.1103/PhysRevC.107.064617⟩
Accession number :
edsair.od......3515..e54222db7a85b14206da9dd0b34faaf7