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Electron-neutrino scattering off nuclei from two different theoretical perspectives

We analyze charged-current electron-neutrino cross sections on Carbon. We consider two different theoretical approaches, on one hand the Continuum Random Phase Approximation (CRPA) which allows a description of giant resonances and quasielastic excitations, on the other hand the RPA-based calculatio...

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Detalles Bibliográficos
Autores principales: Martini, M., Jachowicz, N., Ericson, M., Pandey, V., Van Cuyck, T., Van Dessel, N.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.94.015501
http://cds.cern.ch/record/2128265
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author Martini, M.
Jachowicz, N.
Ericson, M.
Pandey, V.
Van Cuyck, T.
Van Dessel, N.
author_facet Martini, M.
Jachowicz, N.
Ericson, M.
Pandey, V.
Van Cuyck, T.
Van Dessel, N.
author_sort Martini, M.
collection CERN
description We analyze charged-current electron-neutrino cross sections on Carbon. We consider two different theoretical approaches, on one hand the Continuum Random Phase Approximation (CRPA) which allows a description of giant resonances and quasielastic excitations, on the other hand the RPA-based calculations which are able to describe multinucleon emission and coherent and incoherent pion production as well as quasielastic excitations. We compare the two approaches in the genuine quasielastic channel, and find a satisfactory agreement between them at large energies while at low energies the collective giant resonances show up only in the CRPA approach. We also compare electron-neutrino cross sections with the corresponding muon-neutrino ones in order to investigate the impact of the different charged-lepton masses. Finally, restricting to the RPA-based approach we compare the sum of quasielastic, multinucleon emission, coherent and incoherent one-pion production cross sections (folded with the electron-neutrino T2K flux) with the charged-current inclusive electron-neutrino differential cross sections on Carbon measured by T2K. We find a good agreement with the data. The multinucleon component is needed in order to reproduce the T2K electron-neutrino inclusive cross sections.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
record_format invenio
spelling cern-21282652022-08-10T12:38:47Zdoi:10.1103/PhysRevC.94.015501http://cds.cern.ch/record/2128265engMartini, M.Jachowicz, N.Ericson, M.Pandey, V.Van Cuyck, T.Van Dessel, N.Electron-neutrino scattering off nuclei from two different theoretical perspectivesNuclear Physics - TheoryWe analyze charged-current electron-neutrino cross sections on Carbon. We consider two different theoretical approaches, on one hand the Continuum Random Phase Approximation (CRPA) which allows a description of giant resonances and quasielastic excitations, on the other hand the RPA-based calculations which are able to describe multinucleon emission and coherent and incoherent pion production as well as quasielastic excitations. We compare the two approaches in the genuine quasielastic channel, and find a satisfactory agreement between them at large energies while at low energies the collective giant resonances show up only in the CRPA approach. We also compare electron-neutrino cross sections with the corresponding muon-neutrino ones in order to investigate the impact of the different charged-lepton masses. Finally, restricting to the RPA-based approach we compare the sum of quasielastic, multinucleon emission, coherent and incoherent one-pion production cross sections (folded with the electron-neutrino T2K flux) with the charged-current inclusive electron-neutrino differential cross sections on Carbon measured by T2K. We find a good agreement with the data. The multinucleon component is needed in order to reproduce the T2K electron-neutrino inclusive cross sections.We analyze charged-current electron-neutrino cross sections on carbon. We consider two different theoretical approaches, on one hand the continuum random phase approximation (CRPA) which allows a description of giant resonances and quasielastic excitations, on the other hand the RPA-based calculations which are able to describe multinucleon emission and coherent and incoherent pion production as well as quasielastic excitations. We compare the two approaches in the genuine quasielastic channel, and find a satisfactory agreement between them at large energies while at low energies the collective giant resonances show up only in the CRPA approach. We also compare electron-neutrino cross sections with the corresponding muon-neutrino ones in order to investigate the impact of the different charged-lepton masses. Finally, restricting to the RPA-based approach, we compare the sum of quasielastic, multinucleon emission, coherent, and incoherent one-pion production cross sections (folded with the electron-neutrino T2K flux) with the charged-current inclusive electron-neutrino differential cross sections on carbon measured by T2K. We find a good agreement with the data. The multinucleon component is needed in order to reproduce the T2K electron-neutrino inclusive cross sections.We analyze charged-current electron-neutrino cross sections on Carbon. We consider two different theoretical approaches, on one hand the Continuum Random Phase Approximation (CRPA) which allows a description of giant resonances and quasielastic excitations, on the other hand the RPA-based calculations which are able to describe multinucleon emission and coherent and incoherent pion production as well as quasielastic excitations. We compare the two approaches in the genuine quasielastic channel, and find a satisfactory agreement between them at large energies while at low energies the collective giant resonances show up only in the CRPA approach. We also compare electron-neutrino cross sections with the corresponding muon-neutrino ones in order to investigate the impact of the different charged-lepton masses. Finally, restricting to the RPA-based approach we compare the sum of quasielastic, multinucleon emission, coherent and incoherent one-pion production cross sections (folded with the electron-neutrino T2K flux) with the charged-current inclusive electron-neutrino differential cross sections on Carbon measured by T2K. We find a good agreement with the data. The multinucleon component is needed in order to reproduce the T2K electron-neutrino inclusive cross sections.arXiv:1602.00230oai:cds.cern.ch:21282652016-01-31
spellingShingle Nuclear Physics - Theory
Martini, M.
Jachowicz, N.
Ericson, M.
Pandey, V.
Van Cuyck, T.
Van Dessel, N.
Electron-neutrino scattering off nuclei from two different theoretical perspectives
title Electron-neutrino scattering off nuclei from two different theoretical perspectives
title_full Electron-neutrino scattering off nuclei from two different theoretical perspectives
title_fullStr Electron-neutrino scattering off nuclei from two different theoretical perspectives
title_full_unstemmed Electron-neutrino scattering off nuclei from two different theoretical perspectives
title_short Electron-neutrino scattering off nuclei from two different theoretical perspectives
title_sort electron-neutrino scattering off nuclei from two different theoretical perspectives
topic Nuclear Physics - Theory
url https://dx.doi.org/10.1103/PhysRevC.94.015501
http://cds.cern.ch/record/2128265
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AT jachowiczn electronneutrinoscatteringoffnucleifromtwodifferenttheoreticalperspectives
AT ericsonm electronneutrinoscatteringoffnucleifromtwodifferenttheoreticalperspectives
AT pandeyv electronneutrinoscatteringoffnucleifromtwodifferenttheoreticalperspectives
AT vancuyckt electronneutrinoscatteringoffnucleifromtwodifferenttheoreticalperspectives
AT vandesseln electronneutrinoscatteringoffnucleifromtwodifferenttheoreticalperspectives