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Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility
The spent fuel of current nuclear reactors contains fissile plutonium isotopes that can be combined with uranium to make mixed oxide (MOX) fuel. In this way the Pu from spent fuel is used in a new reactor cycle, contributing to the long-term sustainability of nuclear energy. However, an extensive us...
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Lenguaje: | eng |
Publicado: |
2018
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevC.97.024605 http://cds.cern.ch/record/2646875 |
_version_ | 1780960574178328576 |
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author | Lerendegui-Marco, J Guerrero, C Mendoza, E Quesada, J M Eberhardt, K Junghans, A R Krtička, M Aberle, O Andrzejewski, J Audouin, L Bécares, V Bacak, M Balibrea, J Barbagallo, M Barros, S Bečvář, F Beinrucker, C Berthoumieux, E Billowes, J Bosnar, D Brugger, M Caamaño, M Calviño, F Calviani, M Cano-Ott, D Cardella, R Casanovas, A Castelluccio, D M Cerutti, F Chen, Y H Chiaveri, E Colonna, N Cortés, G Cortés-Giraldo, M A Cosentino, L Damone, L A Diakaki, M Dietz, M Domingo-Pardo, C Dressler, R Dupont, E Durán, I Fernández-Domínguez, B Ferrari, A Ferreira, P Finocchiaro, P Furman, V Göbel, K García, A R Gawlik, A Glodariu, T Gonçalves, I F González-Romero, E Goverdovski, A Griesmayer, E Gunsing, F Harada, H Heftrich, T Heinitz, S Heyse, J Jenkins, D G Jericha, E Käppeler, F Kadi, Y Katabuchi, T Kavrigin, P Ketlerov, V Khryachkov, V Kimura, A Kivel, N Kokkoris, M Leal-Cidoncha, E Lederer, C Leeb, H Lo Meo, S Lonsdale, S J Losito, R Macina, D Marganiec, J Martínez, T Massimi, C Mastinu, P Mastromarco, M Matteucci, F Maugeri, E A Mengoni, A Milazzo, P M Mingrone, F Mirea, M Montesano, S Musumarra, A Nolte, R Oprea, A Patronis, N Pavlik, A Perkowski, J Porras, J I Praena, J Rajeev, K Rauscher, T Reifarth, R Riego-Perez, A Rout, P C Rubbia, C Ryan, J A Sabaté-Gilarte, M Saxena, A Schillebeeckx, P Schmidt, S Schumann, D Sedyshev, P Smith, A G Stamatopoulos, A Tagliente, G Tain, J L Tarifeño-Saldivia, A Tassan-Got, L Tsinganis, A Valenta, S Vannini, G Variale, V Vaz, P Ventura, A Vlachoudis, V Vlastou, R Wallner, A Warren, S Weigand, M Weiss, C Wolf, C Woods, P J Wright, T Žugec, P |
author_facet | Lerendegui-Marco, J Guerrero, C Mendoza, E Quesada, J M Eberhardt, K Junghans, A R Krtička, M Aberle, O Andrzejewski, J Audouin, L Bécares, V Bacak, M Balibrea, J Barbagallo, M Barros, S Bečvář, F Beinrucker, C Berthoumieux, E Billowes, J Bosnar, D Brugger, M Caamaño, M Calviño, F Calviani, M Cano-Ott, D Cardella, R Casanovas, A Castelluccio, D M Cerutti, F Chen, Y H Chiaveri, E Colonna, N Cortés, G Cortés-Giraldo, M A Cosentino, L Damone, L A Diakaki, M Dietz, M Domingo-Pardo, C Dressler, R Dupont, E Durán, I Fernández-Domínguez, B Ferrari, A Ferreira, P Finocchiaro, P Furman, V Göbel, K García, A R Gawlik, A Glodariu, T Gonçalves, I F González-Romero, E Goverdovski, A Griesmayer, E Gunsing, F Harada, H Heftrich, T Heinitz, S Heyse, J Jenkins, D G Jericha, E Käppeler, F Kadi, Y Katabuchi, T Kavrigin, P Ketlerov, V Khryachkov, V Kimura, A Kivel, N Kokkoris, M Leal-Cidoncha, E Lederer, C Leeb, H Lo Meo, S Lonsdale, S J Losito, R Macina, D Marganiec, J Martínez, T Massimi, C Mastinu, P Mastromarco, M Matteucci, F Maugeri, E A Mengoni, A Milazzo, P M Mingrone, F Mirea, M Montesano, S Musumarra, A Nolte, R Oprea, A Patronis, N Pavlik, A Perkowski, J Porras, J I Praena, J Rajeev, K Rauscher, T Reifarth, R Riego-Perez, A Rout, P C Rubbia, C Ryan, J A Sabaté-Gilarte, M Saxena, A Schillebeeckx, P Schmidt, S Schumann, D Sedyshev, P Smith, A G Stamatopoulos, A Tagliente, G Tain, J L Tarifeño-Saldivia, A Tassan-Got, L Tsinganis, A Valenta, S Vannini, G Variale, V Vaz, P Ventura, A Vlachoudis, V Vlastou, R Wallner, A Warren, S Weigand, M Weiss, C Wolf, C Woods, P J Wright, T Žugec, P |
author_sort | Lerendegui-Marco, J |
collection | CERN |
description | The spent fuel of current nuclear reactors contains fissile plutonium isotopes that can be combined with uranium to make mixed oxide (MOX) fuel. In this way the Pu from spent fuel is used in a new reactor cycle, contributing to the long-term sustainability of nuclear energy. However, an extensive use of MOX fuels, in particular in fast reactors, requires more accurate capture and fission cross sections for some Pu isotopes. In the case of $^{242}$Pu there are sizable discrepancies among the existing capture cross-section measurements included in the evaluations (all from the 1970s) resulting in an uncertainty as high as 35% in the fast energy region. Moreover, postirradiation experiments evaluated with JEFF-3.1 indicate an overestimation of 14% in the capture cross section in the fast neutron energy region. In this context, the Nuclear Energy Agency (NEA) requested an accuracy of 8% in this cross section in the energy region between 500 meV and 500 keV. This paper presents a new time-of-flight capture measurement on $^{242}$Pu carried out at n_TOF-EAR1 (CERN), focusing on the analysis and statistical properties of the resonance region, below 4 keV. The $^{242}$Pu(n,$\gamma$) reaction on a sample containing 95(4) mg enriched to 99.959% was measured with an array of four C$_6$D$_6$ detectors and applying the total energy detection technique. The high neutron energy resolution of n_TOF-EAR1 and the good statistics accumulated have allowed us to extend the resonance analysis up to 4 keV, obtaining new individual and average resonance parameters from a capture cross section featuring a systematic uncertainty of 5%, fulfilling the request of the NEA. |
id | oai-inspirehep.net-1654298 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2018 |
record_format | invenio |
spelling | oai-inspirehep.net-16542982021-05-03T08:12:24Zdoi:10.1103/PhysRevC.97.024605http://cds.cern.ch/record/2646875engLerendegui-Marco, JGuerrero, CMendoza, EQuesada, J MEberhardt, KJunghans, A RKrtička, MAberle, OAndrzejewski, JAudouin, LBécares, VBacak, MBalibrea, JBarbagallo, MBarros, SBečvář, FBeinrucker, CBerthoumieux, EBillowes, JBosnar, DBrugger, MCaamaño, MCalviño, FCalviani, MCano-Ott, DCardella, RCasanovas, ACastelluccio, D MCerutti, FChen, Y HChiaveri, EColonna, NCortés, GCortés-Giraldo, M ACosentino, LDamone, L ADiakaki, MDietz, MDomingo-Pardo, CDressler, RDupont, EDurán, IFernández-Domínguez, BFerrari, AFerreira, PFinocchiaro, PFurman, VGöbel, KGarcía, A RGawlik, AGlodariu, TGonçalves, I FGonzález-Romero, EGoverdovski, AGriesmayer, EGunsing, FHarada, HHeftrich, THeinitz, SHeyse, JJenkins, D GJericha, EKäppeler, FKadi, YKatabuchi, TKavrigin, PKetlerov, VKhryachkov, VKimura, AKivel, NKokkoris, MLeal-Cidoncha, ELederer, CLeeb, HLo Meo, SLonsdale, S JLosito, RMacina, DMarganiec, JMartínez, TMassimi, CMastinu, PMastromarco, MMatteucci, FMaugeri, E AMengoni, AMilazzo, P MMingrone, FMirea, MMontesano, SMusumarra, ANolte, ROprea, APatronis, NPavlik, APerkowski, JPorras, J IPraena, JRajeev, KRauscher, TReifarth, RRiego-Perez, ARout, P CRubbia, CRyan, J ASabaté-Gilarte, MSaxena, ASchillebeeckx, PSchmidt, SSchumann, DSedyshev, PSmith, A GStamatopoulos, ATagliente, GTain, J LTarifeño-Saldivia, ATassan-Got, LTsinganis, AValenta, SVannini, GVariale, VVaz, PVentura, AVlachoudis, VVlastou, RWallner, AWarren, SWeigand, MWeiss, CWolf, CWoods, P JWright, TŽugec, PRadiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facilityNuclear Physics - ExperimentThe spent fuel of current nuclear reactors contains fissile plutonium isotopes that can be combined with uranium to make mixed oxide (MOX) fuel. In this way the Pu from spent fuel is used in a new reactor cycle, contributing to the long-term sustainability of nuclear energy. However, an extensive use of MOX fuels, in particular in fast reactors, requires more accurate capture and fission cross sections for some Pu isotopes. In the case of $^{242}$Pu there are sizable discrepancies among the existing capture cross-section measurements included in the evaluations (all from the 1970s) resulting in an uncertainty as high as 35% in the fast energy region. Moreover, postirradiation experiments evaluated with JEFF-3.1 indicate an overestimation of 14% in the capture cross section in the fast neutron energy region. In this context, the Nuclear Energy Agency (NEA) requested an accuracy of 8% in this cross section in the energy region between 500 meV and 500 keV. This paper presents a new time-of-flight capture measurement on $^{242}$Pu carried out at n_TOF-EAR1 (CERN), focusing on the analysis and statistical properties of the resonance region, below 4 keV. The $^{242}$Pu(n,$\gamma$) reaction on a sample containing 95(4) mg enriched to 99.959% was measured with an array of four C$_6$D$_6$ detectors and applying the total energy detection technique. The high neutron energy resolution of n_TOF-EAR1 and the good statistics accumulated have allowed us to extend the resonance analysis up to 4 keV, obtaining new individual and average resonance parameters from a capture cross section featuring a systematic uncertainty of 5%, fulfilling the request of the NEA.oai:inspirehep.net:16542982018 |
spellingShingle | Nuclear Physics - Experiment Lerendegui-Marco, J Guerrero, C Mendoza, E Quesada, J M Eberhardt, K Junghans, A R Krtička, M Aberle, O Andrzejewski, J Audouin, L Bécares, V Bacak, M Balibrea, J Barbagallo, M Barros, S Bečvář, F Beinrucker, C Berthoumieux, E Billowes, J Bosnar, D Brugger, M Caamaño, M Calviño, F Calviani, M Cano-Ott, D Cardella, R Casanovas, A Castelluccio, D M Cerutti, F Chen, Y H Chiaveri, E Colonna, N Cortés, G Cortés-Giraldo, M A Cosentino, L Damone, L A Diakaki, M Dietz, M Domingo-Pardo, C Dressler, R Dupont, E Durán, I Fernández-Domínguez, B Ferrari, A Ferreira, P Finocchiaro, P Furman, V Göbel, K García, A R Gawlik, A Glodariu, T Gonçalves, I F González-Romero, E Goverdovski, A Griesmayer, E Gunsing, F Harada, H Heftrich, T Heinitz, S Heyse, J Jenkins, D G Jericha, E Käppeler, F Kadi, Y Katabuchi, T Kavrigin, P Ketlerov, V Khryachkov, V Kimura, A Kivel, N Kokkoris, M Leal-Cidoncha, E Lederer, C Leeb, H Lo Meo, S Lonsdale, S J Losito, R Macina, D Marganiec, J Martínez, T Massimi, C Mastinu, P Mastromarco, M Matteucci, F Maugeri, E A Mengoni, A Milazzo, P M Mingrone, F Mirea, M Montesano, S Musumarra, A Nolte, R Oprea, A Patronis, N Pavlik, A Perkowski, J Porras, J I Praena, J Rajeev, K Rauscher, T Reifarth, R Riego-Perez, A Rout, P C Rubbia, C Ryan, J A Sabaté-Gilarte, M Saxena, A Schillebeeckx, P Schmidt, S Schumann, D Sedyshev, P Smith, A G Stamatopoulos, A Tagliente, G Tain, J L Tarifeño-Saldivia, A Tassan-Got, L Tsinganis, A Valenta, S Vannini, G Variale, V Vaz, P Ventura, A Vlachoudis, V Vlastou, R Wallner, A Warren, S Weigand, M Weiss, C Wolf, C Woods, P J Wright, T Žugec, P Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title | Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title_full | Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title_fullStr | Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title_full_unstemmed | Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title_short | Radiative neutron capture on $^{242}\mathrm{Pu}$ in the resonance region at the CERN n_TOF-EAR1 facility |
title_sort | radiative neutron capture on $^{242}\mathrm{pu}$ in the resonance region at the cern n_tof-ear1 facility |
topic | Nuclear Physics - Experiment |
url | https://dx.doi.org/10.1103/PhysRevC.97.024605 http://cds.cern.ch/record/2646875 |
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radiativeneutroncaptureon242mathrmpuintheresonanceregionatthecernntofear1facility AT wrightt radiativeneutroncaptureon242mathrmpuintheresonanceregionatthecernntofear1facility AT zugecp radiativeneutroncaptureon242mathrmpuintheresonanceregionatthecernntofear1facility |