Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission

Detalhes bibliográficos
Autor(a) principal: ANDRADE-II, E.
Data de Publicação: 2017
Outros Autores: MENEZES, J.C.M., DUARTE, S.B., GARCIA, F., ROSSI, P.C.R., TAVARES, O.A.P., DEPPMAN, A., INTERNATIONAL WORKSHOP ON COMPOUND NUCLEAR REACTIONS AND RELATED TOPICS, 3rd
Tipo de documento: Artigo de conferência
Título da fonte: Repositório Institucional do IPEN
Texto Completo: http://repositorio.ipen.br/handle/123456789/27623
Resumo: We study the effects of fissioning nuclei mass- and energy-distributions on the formation of fragments for fission induced by high energy probes. A Monte Carlo code called CRISP was used for obtaining mass distributions and spectra of the fissioning nuclei for reactions induced by 660 MeV protons on 241Am and on 239Np, by 500 MeV protons on 208Pb, and by Bremsstrahlung photons with end-point energies at 50 MeV and 3500 MeV on 238U. The results show that even at high excitation energies, asymmetric fission may still contribute significantly to the fission cross section of actinide nuclei, while it is the dominante mode in the case of lead. However, more precise data for high energy fission on actinide are necessary in order to allow definite conclusions.
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spelling 2017-07-05T18:18:07Z2017-07-05T18:18:07ZSeptember 19-23, 2011http://repositorio.ipen.br/handle/123456789/2762310.1051/epjconf/20122110001We study the effects of fissioning nuclei mass- and energy-distributions on the formation of fragments for fission induced by high energy probes. A Monte Carlo code called CRISP was used for obtaining mass distributions and spectra of the fissioning nuclei for reactions induced by 660 MeV protons on 241Am and on 239Np, by 500 MeV protons on 208Pb, and by Bremsstrahlung photons with end-point energies at 50 MeV and 3500 MeV on 238U. The results show that even at high excitation energies, asymmetric fission may still contribute significantly to the fission cross section of actinide nuclei, while it is the dominante mode in the case of lead. However, more precise data for high energy fission on actinide are necessary in order to allow definite conclusions.Submitted by Marco Antonio Oliveira da Silva (maosilva@ipen.br) on 2017-07-05T18:18:07Z No. of bitstreams: 1 23854.pdf: 699969 bytes, checksum: 34d3b79b0bc45fcb920e1c0358eff5cd (MD5)Made available in DSpace on 2017-07-05T18:18:07Z (GMT). No. of bitstreams: 1 23854.pdf: 699969 bytes, checksum: 34d3b79b0bc45fcb920e1c0358eff5cd (MD5)1-9EDP SciencesEPJ Web of Conferences, 21, 10001Effects of fissioning nuclei distributions on fragment mass distributions for high energy fissioninfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/conferenceObjectILes Ulis, FrancePrague, Czech RepublicANDRADE-II, E.MENEZES, J.C.M.DUARTE, S.B.GARCIA, F.ROSSI, P.C.R.TAVARES, O.A.P.DEPPMAN, A.INTERNATIONAL WORKSHOP ON COMPOUND NUCLEAR REACTIONS AND RELATED TOPICS, 3rdinfo:eu-repo/semantics/openAccessreponame:Repositório Institucional do IPENinstname:Instituto de Pesquisas Energéticas e Nucleares (IPEN)instacron:IPEN238542012ROSSI, P.C.R.17-07Proceedings40467533787ROSSI, P.C.R.:4046:450:NTAVARES, O.A.P.:7533:-1:NDEPPMAN, A.:787:-1:NORIGINAL23854.pdf23854.pdfapplication/pdf699969http://repositorio.ipen.br/bitstream/123456789/27623/1/23854.pdf34d3b79b0bc45fcb920e1c0358eff5cdMD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://repositorio.ipen.br/bitstream/123456789/27623/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52123456789/276232017-07-05 18:18:07.829oai:repositorio.ipen.br:123456789/27623Tk9URTogUExBQ0UgWU9VUiBPV04gTElDRU5TRSBIRVJFClRoaXMgc2FtcGxlIGxpY2Vuc2UgaXMgcHJvdmlkZWQgZm9yIGluZm9ybWF0aW9uYWwgcHVycG9zZXMgb25seS4KCk5PTi1FWENMVVNJVkUgRElTVFJJQlVUSU9OIExJQ0VOU0UKCkJ5IHNpZ25pbmcgYW5kIHN1Ym1pdHRpbmcgdGhpcyBsaWNlbnNlLCB5b3UgKHRoZSBhdXRob3Iocykgb3IgY29weXJpZ2h0Cm93bmVyKSBncmFudHMgdG8gRFNwYWNlIFVuaXZlcnNpdHkgKERTVSkgdGhlIG5vbi1leGNsdXNpdmUgcmlnaHQgdG8gcmVwcm9kdWNlLAp0cmFuc2xhdGUgKGFzIGRlZmluZWQgYmVsb3cpLCBhbmQvb3IgZGlzdHJpYnV0ZSB5b3VyIHN1Ym1pc3Npb24gKGluY2x1ZGluZwp0aGUgYWJzdHJhY3QpIHdvcmxkd2lkZSBpbiBwcmludCBhbmQgZWxlY3Ryb25pYyBmb3JtYXQgYW5kIGluIGFueSBtZWRpdW0sCmluY2x1ZGluZyBidXQgbm90IGxpbWl0ZWQgdG8gYXVkaW8gb3IgdmlkZW8uCgpZb3UgYWdyZWUgdGhhdCBEU1UgbWF5LCB3aXRob3V0IGNoYW5naW5nIHRoZSBjb250ZW50LCB0cmFuc2xhdGUgdGhlCnN1Ym1pc3Npb24gdG8gYW55IG1lZGl1bSBvciBmb3JtYXQgZm9yIHRoZSBwdXJwb3NlIG9mIHByZXNlcnZhdGlvbi4KCllvdSBhbHNvIGFncmVlIHRoYXQgRFNVIG1heSBrZWVwIG1vcmUgdGhhbiBvbmUgY29weSBvZiB0aGlzIHN1Ym1pc3Npb24gZm9yCnB1cnBvc2VzIG9mIHNlY3VyaXR5LCBiYWNrLXVwIGFuZCBwcmVzZXJ2YXRpb24uCgpZb3UgcmVwcmVzZW50IHRoYXQgdGhlIHN1Ym1pc3Npb24gaXMgeW91ciBvcmlnaW5hbCB3b3JrLCBhbmQgdGhhdCB5b3UgaGF2ZQp0aGUgcmlnaHQgdG8gZ3JhbnQgdGhlIHJpZ2h0cyBjb250YWluZWQgaW4gdGhpcyBsaWNlbnNlLiBZb3UgYWxzbyByZXByZXNlbnQKdGhhdCB5b3VyIHN1Ym1pc3Npb24gZG9lcyBub3QsIHRvIHRoZSBiZXN0IG9mIHlvdXIga25vd2xlZGdlLCBpbmZyaW5nZSB1cG9uCmFueW9uZSdzIGNvcHlyaWdodC4KCklmIHRoZSBzdWJtaXNzaW9uIGNvbnRhaW5zIG1hdGVyaWFsIGZvciB3aGljaCB5b3UgZG8gbm90IGhvbGQgY29weXJpZ2h0LAp5b3UgcmVwcmVzZW50IHRoYXQgeW91IGhhdmUgb2J0YWluZWQgdGhlIHVucmVzdHJpY3RlZCBwZXJtaXNzaW9uIG9mIHRoZQpjb3B5cmlnaHQgb3duZXIgdG8gZ3JhbnQgRFNVIHRoZSByaWdodHMgcmVxdWlyZWQgYnkgdGhpcyBsaWNlbnNlLCBhbmQgdGhhdApzdWNoIHRoaXJkLXBhcnR5IG93bmVkIG1hdGVyaWFsIGlzIGNsZWFybHkgaWRlbnRpZmllZCBhbmQgYWNrbm93bGVkZ2VkCndpdGhpbiB0aGUgdGV4dCBvciBjb250ZW50IG9mIHRoZSBzdWJtaXNzaW9uLgoKSUYgVEhFIFNVQk1JU1NJT04gSVMgQkFTRUQgVVBPTiBXT1JLIFRIQVQgSEFTIEJFRU4gU1BPTlNPUkVEIE9SIFNVUFBPUlRFRApCWSBBTiBBR0VOQ1kgT1IgT1JHQU5JWkFUSU9OIE9USEVSIFRIQU4gRFNVLCBZT1UgUkVQUkVTRU5UIFRIQVQgWU9VIEhBVkUKRlVMRklMTEVEIEFOWSBSSUdIVCBPRiBSRVZJRVcgT1IgT1RIRVIgT0JMSUdBVElPTlMgUkVRVUlSRUQgQlkgU1VDSApDT05UUkFDVCBPUiBBR1JFRU1FTlQuCgpEU1Ugd2lsbCBjbGVhcmx5IGlkZW50aWZ5IHlvdXIgbmFtZShzKSBhcyB0aGUgYXV0aG9yKHMpIG9yIG93bmVyKHMpIG9mIHRoZQpzdWJtaXNzaW9uLCBhbmQgd2lsbCBub3QgbWFrZSBhbnkgYWx0ZXJhdGlvbiwgb3RoZXIgdGhhbiBhcyBhbGxvd2VkIGJ5IHRoaXMKbGljZW5zZSwgdG8geW91ciBzdWJtaXNzaW9uLgo=Repositório InstitucionalPUBhttp://repositorio.ipen.br/oai/requestbibl@ipen.bropendoar:45102017-07-05T18:18:07Repositório Institucional do IPEN - Instituto de Pesquisas Energéticas e Nucleares (IPEN)false
dc.title.pt_BR.fl_str_mv Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
title Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
spellingShingle Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
ANDRADE-II, E.
title_short Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
title_full Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
title_fullStr Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
title_full_unstemmed Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
title_sort Effects of fissioning nuclei distributions on fragment mass distributions for high energy fission
author ANDRADE-II, E.
author_facet ANDRADE-II, E.
MENEZES, J.C.M.
DUARTE, S.B.
GARCIA, F.
ROSSI, P.C.R.
TAVARES, O.A.P.
DEPPMAN, A.
INTERNATIONAL WORKSHOP ON COMPOUND NUCLEAR REACTIONS AND RELATED TOPICS, 3rd
author_role author
author2 MENEZES, J.C.M.
DUARTE, S.B.
GARCIA, F.
ROSSI, P.C.R.
TAVARES, O.A.P.
DEPPMAN, A.
INTERNATIONAL WORKSHOP ON COMPOUND NUCLEAR REACTIONS AND RELATED TOPICS, 3rd
author2_role author
author
author
author
author
author
author
dc.contributor.author.fl_str_mv ANDRADE-II, E.
MENEZES, J.C.M.
DUARTE, S.B.
GARCIA, F.
ROSSI, P.C.R.
TAVARES, O.A.P.
DEPPMAN, A.
INTERNATIONAL WORKSHOP ON COMPOUND NUCLEAR REACTIONS AND RELATED TOPICS, 3rd
description We study the effects of fissioning nuclei mass- and energy-distributions on the formation of fragments for fission induced by high energy probes. A Monte Carlo code called CRISP was used for obtaining mass distributions and spectra of the fissioning nuclei for reactions induced by 660 MeV protons on 241Am and on 239Np, by 500 MeV protons on 208Pb, and by Bremsstrahlung photons with end-point energies at 50 MeV and 3500 MeV on 238U. The results show that even at high excitation energies, asymmetric fission may still contribute significantly to the fission cross section of actinide nuclei, while it is the dominante mode in the case of lead. However, more precise data for high energy fission on actinide are necessary in order to allow definite conclusions.
publishDate 2017
dc.date.evento.pt_BR.fl_str_mv September 19-23, 2011
dc.date.accessioned.fl_str_mv 2017-07-05T18:18:07Z
dc.date.available.fl_str_mv 2017-07-05T18:18:07Z
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dc.identifier.uri.fl_str_mv http://repositorio.ipen.br/handle/123456789/27623
dc.identifier.doi.pt_BR.fl_str_mv 10.1051/epjconf/20122110001
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identifier_str_mv 10.1051/epjconf/20122110001
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