Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV

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A study of charged-current muon neutrino scattering on hydrocarbon (CH) in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from q...

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oai_identifier_str oai:repositorio.concytec.gob.pe:20.500.12390/1103
network_acronym_str CONC
network_name_str CONCYTEC-Institucional
repository_id_str 4689
dc.title.none.fl_str_mv Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
title Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
spellingShingle Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
Walton, T
Neutrino physics
Nuclear interactions
Particle physics
Charged-current muon neutrino scattering
Quasielastic and inelastic processes
Hydrocarbon (CH) target
title_short Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
title_full Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
title_fullStr Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
title_full_unstemmed Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
title_sort Measurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeV
author Walton, T
author_facet Walton, T
Betancourt, M
Aliaga, L
Altinok, O
Bodek, A
Bravar, A
Budd, H
Bustamante, MJ
Butkevich, A
Caicedo, DAM
Carneiro, MF
Castromonte, CM
Christy, ME
Chvojka, J
da Motta, H
Datta, M
Devan, J
Dytman, SA
Diaz, GA
Eberly, B
Felix, J
Fields, L
Fine, R
Fiorentini, GA
Gago, AM
Gallagher, H
Gran, R
Harris, DA
Higuera, A
Hurtado, K
Kleykamp, J
Kordosky, M
Kulagin, SA
Le, T
Maher, E
Manly, S
Mann, WA
Marshall, CM
Mari, CM
McFarland, KS
McGivern, CL
McGowan, AM
Messerly, B
Miller, J
Mislivec, A
Morfin, JG
Mousseau, J
Muhlbeier, T
Naples, D
Nelson, JK
Norrick, A
Osta, J
Paolone, V
Park, J
Patrick, CE
Perdue, GN
Rakotondravohitra, L
Ransome, RD
Ray, H
Ren, L
Rodrigues, PA
Ruterbories, D
Schellman, H
Schmitz, DW
Simon, C
Snider, FD
Sobczyk, JT
Salinas, CJS
Tagg, N
Tice, BG
Valencia, E
Wolcott, J
Wospakrik, M
Zavala, G
Zhang, D
Ziemer, BP
author_role author
author2 Betancourt, M
Aliaga, L
Altinok, O
Bodek, A
Bravar, A
Budd, H
Bustamante, MJ
Butkevich, A
Caicedo, DAM
Carneiro, MF
Castromonte, CM
Christy, ME
Chvojka, J
da Motta, H
Datta, M
Devan, J
Dytman, SA
Diaz, GA
Eberly, B
Felix, J
Fields, L
Fine, R
Fiorentini, GA
Gago, AM
Gallagher, H
Gran, R
Harris, DA
Higuera, A
Hurtado, K
Kleykamp, J
Kordosky, M
Kulagin, SA
Le, T
Maher, E
Manly, S
Mann, WA
Marshall, CM
Mari, CM
McFarland, KS
McGivern, CL
McGowan, AM
Messerly, B
Miller, J
Mislivec, A
Morfin, JG
Mousseau, J
Muhlbeier, T
Naples, D
Nelson, JK
Norrick, A
Osta, J
Paolone, V
Park, J
Patrick, CE
Perdue, GN
Rakotondravohitra, L
Ransome, RD
Ray, H
Ren, L
Rodrigues, PA
Ruterbories, D
Schellman, H
Schmitz, DW
Simon, C
Snider, FD
Sobczyk, JT
Salinas, CJS
Tagg, N
Tice, BG
Valencia, E
Wolcott, J
Wospakrik, M
Zavala, G
Zhang, D
Ziemer, BP
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dc.contributor.author.fl_str_mv Walton, T
Betancourt, M
Aliaga, L
Altinok, O
Bodek, A
Bravar, A
Budd, H
Bustamante, MJ
Butkevich, A
Caicedo, DAM
Carneiro, MF
Castromonte, CM
Christy, ME
Chvojka, J
da Motta, H
Datta, M
Devan, J
Dytman, SA
Diaz, GA
Eberly, B
Felix, J
Fields, L
Fine, R
Fiorentini, GA
Gago, AM
Gallagher, H
Gran, R
Harris, DA
Higuera, A
Hurtado, K
Kleykamp, J
Kordosky, M
Kulagin, SA
Le, T
Maher, E
Manly, S
Mann, WA
Marshall, CM
Mari, CM
McFarland, KS
McGivern, CL
McGowan, AM
Messerly, B
Miller, J
Mislivec, A
Morfin, JG
Mousseau, J
Muhlbeier, T
Naples, D
Nelson, JK
Norrick, A
Osta, J
Paolone, V
Park, J
Patrick, CE
Perdue, GN
Rakotondravohitra, L
Ransome, RD
Ray, H
Ren, L
Rodrigues, PA
Ruterbories, D
Schellman, H
Schmitz, DW
Simon, C
Snider, FD
Sobczyk, JT
Salinas, CJS
Tagg, N
Tice, BG
Valencia, E
Wolcott, J
Wospakrik, M
Zavala, G
Zhang, D
Ziemer, BP
dc.subject.en.fl_str_mv Neutrino physics
Nuclear interactions
Particle physics
Charged-current muon neutrino scattering
Quasielastic and inelastic processes
Hydrocarbon (CH) target
topic Neutrino physics
Nuclear interactions
Particle physics
Charged-current muon neutrino scattering
Quasielastic and inelastic processes
Hydrocarbon (CH) target
description A study of charged-current muon neutrino scattering on hydrocarbon (CH) in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70◦ and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well-described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multi-nucleon correlations. This measurement guides the formulation of a complete description of neutrino-nucleus interactions that encompasses the hadronic as well as the leptonic aspects of this process.
publishDate 2015
dc.date.accessioned.none.fl_str_mv 2024-05-30T23:13:38Z
dc.date.available.none.fl_str_mv 2024-05-30T23:13:38Z
dc.date.issued.fl_str_mv 2015
dc.type.none.fl_str_mv info:eu-repo/semantics/article
format article
dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/20.500.12390/1103
dc.identifier.doi.none.fl_str_mv https://doi.org/10.1103/PhysRevD.91.071301
dc.identifier.isi.none.fl_str_mv 352130200001
url https://hdl.handle.net/20.500.12390/1103
https://doi.org/10.1103/PhysRevD.91.071301
identifier_str_mv 352130200001
dc.language.iso.none.fl_str_mv eng
language eng
dc.relation.ispartof.none.fl_str_mv Physical Review D
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.uri.none.fl_str_mv https://creativecommons.org/licenses/by/4.0/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by/4.0/
dc.publisher.en.fl_str_mv American Physical Society
American Physical Society
dc.source.none.fl_str_mv reponame:CONCYTEC-Institucional
instname:Consejo Nacional de Ciencia Tecnología e Innovación
instacron:CONCYTEC
instname_str Consejo Nacional de Ciencia Tecnología e Innovación
instacron_str CONCYTEC
institution CONCYTEC
reponame_str CONCYTEC-Institucional
collection CONCYTEC-Institucional
repository.name.fl_str_mv Repositorio Institucional CONCYTEC
repository.mail.fl_str_mv repositorio@concytec.gob.pe
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Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70◦ and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well-described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multi-nucleon correlations. This measurement guides the formulation of a complete description of neutrino-nucleus interactions that encompasses the hadronic as well as the leptonic aspects of this process.A study of charged-current muon neutrino scattering on hydrocarbon in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70 degrees and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multinucleon correlations. This measurement guides the formulation of a complete description of neutrino-nucleus interactions that encompasses the hadronic as well as the leptonic aspects of this process.Consejo Nacional de Ciencia, Tecnología e Innovación Tecnológica - ConcytecengAmerican Physical SocietyAmerican Physical SocietyPhysical Review Dinfo:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by/4.0/Neutrino physicsNuclear interactionsParticle physicsCharged-current muon neutrino scatteringQuasielastic and inelastic processesHydrocarbon (CH) targetMeasurement of muon plus proton final states in nu(mu) interactions on hydrocarbon at < E-nu >=4.2 GeVinfo:eu-repo/semantics/articlereponame:CONCYTEC-Institucionalinstname:Consejo Nacional de Ciencia Tecnología e 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<DisplayName>Wolcott, J</DisplayName> <Person id="rp00822" /> <Affiliation> <OrgUnit> </OrgUnit> </Affiliation> </Author> <Author> <DisplayName>Wospakrik, M</DisplayName> <Person id="rp00782" /> <Affiliation> <OrgUnit> </OrgUnit> </Affiliation> </Author> <Author> <DisplayName>Zavala, G</DisplayName> <Person id="rp01268" /> <Affiliation> <OrgUnit> </OrgUnit> </Affiliation> </Author> <Author> <DisplayName>Zhang, D</DisplayName> <Person id="rp00853" /> <Affiliation> <OrgUnit> </OrgUnit> </Affiliation> </Author> <Author> <DisplayName>Ziemer, BP</DisplayName> <Person id="rp00860" /> <Affiliation> <OrgUnit> </OrgUnit> </Affiliation> </Author> </Authors> <Editors> </Editors> <Publishers> <Publisher> <DisplayName>American Physical Society</DisplayName> <DisplayName>American Physical Society</DisplayName> <OrgUnit /> </Publisher> </Publishers> <License>https://creativecommons.org/licenses/by/4.0/</License> <Keyword>Neutrino physics</Keyword> <Keyword>Nuclear interactions</Keyword> <Keyword>Particle physics</Keyword> <Keyword>Charged-current muon neutrino scattering</Keyword> <Keyword>Quasielastic and inelastic processes</Keyword> <Keyword>Hydrocarbon (CH) target</Keyword> <Abstract>A study of charged-current muon neutrino scattering on hydrocarbon (CH) in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70◦ and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well-described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multi-nucleon correlations. This measurement guides the formulation of a complete description of neutrino-nucleus interactions that encompasses the hadronic as well as the leptonic aspects of this process.</Abstract> <Abstract>A study of charged-current muon neutrino scattering on hydrocarbon in which the final state includes a muon, at least one proton, and no pions is presented. Although this signature has the topology of neutrino quasielastic scattering from neutrons, the event sample contains contributions from quasielastic and inelastic processes where pions are absorbed in the nucleus. The analysis accepts events with muon production angles up to 70 degrees and proton kinetic energies greater than 110 MeV. The cross section, when based completely on hadronic kinematics, is well described by a relativistic Fermi gas nuclear model including the neutrino event generator modeling for inelastic processes and particle transportation through the nucleus. This is in contrast to the quasielastic cross section based on muon kinematics, which is best described by an extended model that incorporates multinucleon correlations. This measurement guides the formulation of a complete description of neutrino-nucleus interactions that encompasses the hadronic as well as the leptonic aspects of this process.</Abstract> <Access xmlns="http://purl.org/coar/access_right" > </Access> </Publication> -1
score 13.836569
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