Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV

T. Walton; M. Betancourt; L. Aliaga; O. Altinok; A. Bodek; A. Bravar; H. Budd; M. Bustamante; A. Butkevich; D. A. Martinez Caicedo; M. F. Carneiro; C. M. Castromonte; M. E. Christy; J. Chvojka; H. Da Motta; M. Datta; J. Devan; S. A. Dytman; G. A. Díaz; B. Eberly; J. Felix; L. Fields; R. Fine; G. A. Fiorentini; A. Gago; H. Gallagher; R. Gran; D. A. Harris; A. Higuera; K. Hurtado; J. Kleykamp; M. Kordosky; S. A. Kulagin; T. Le; E. Maher; S. Manly; W. A. Mann; C. M. Marshall; C. Martin Mari; K. S. McFarland; C. L. McGivern; A. M. McGowan; B. Messerly; J. Miller; A. Mislivec; J. G. Morfín; J. Mousseau; T. Muhlbeier; D. Naples; J. K. Nelson; A. Norrick; J. Osta; V. Paolone; J. Park; C. E. Patrick; G. N. Perdue; L. Rakotondravohitra; R. D. Ransome; H. Ray; L. Ren; P. A. Rodrigues; D. Ruterbories; H. Schellman; D. W. Schmitz; C. Simon; F. D. Snider; J. T. Sobczyk; C. J. Solano Salinas; N. Tagg; B. G. Tice; E. Valencia; J. Wolcott; M. Wospakrik; G. Zavala; D. Zhang; B. P. Ziemer

Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV

T. Walton, M. Betancourt, L. Aliaga, O. Altinok, A. Bodek, A. Bravar, H. Budd, M. Bustamante, A. Butkevich, D. A. Martinez Caicedo, M. F. Carneiro, C. M. Castromonte, M. E. Christy, J. Chvojka, H. Da Motta, M. Datta, J. Devan, S. A. Dytman, G. A. Díaz, B. EberlyJ. Felix, L. Fields, R. Fine, G. A. Fiorentini, A. Gago, H. Gallagher, R. Gran, D. A. Harris, A. Higuera, K. Hurtado, J. Kleykamp, M. Kordosky, S. A. Kulagin, T. Le, E. Maher, S. Manly, W. A. Mann, C. M. Marshall, C. Martin Mari, K. S. McFarland, C. L. McGivern, A. M. McGowan, B. Messerly, J. Miller, A. Mislivec, J. G. Morfín, J. Mousseau, T. Muhlbeier, D. Naples, J. K. Nelson, A. Norrick, J. Osta, V. Paolone, J. Park, C. E. Patrick, G. N. Perdue, L. Rakotondravohitra, R. D. Ransome, H. Ray, L. Ren, P. A. Rodrigues, D. Ruterbories, H. Schellman, D. W. Schmitz, C. Simon, F. D. Snider, J. T. Sobczyk, C. J. Solano Salinas, N. Tagg, B. G. Tice, E. Valencia, J. Wolcott, M. Wospakrik, G. Zavala, D. Zhang, B. P. Ziemer

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53 Citas (Scopus)

Resumen

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° 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.

Idioma original	Español
Publicación	Physical Review D - Particles, Fields, Gravitation and Cosmology
Volumen	91
Estado	Publicada - 1 abr. 2015

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Walton, T., Betancourt, M., Aliaga, L., Altinok, O., Bodek, A., Bravar, A., Budd, H., Bustamante, M., Butkevich, A., Martinez Caicedo, D. A., Carneiro, M. F., Castromonte, C. M., Christy, M. E., Chvojka, J., Da Motta, H., Datta, M., Devan, J., Dytman, S. A., Díaz, G. A., ... Ziemer, B. P. (2015). Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV. Physical Review D - Particles, Fields, Gravitation and Cosmology, 91.

@article{14c4939f9d8845848cc5419bafe07b0d,

title = "Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV",

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° 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.",

author = "T. Walton and M. Betancourt and L. Aliaga and O. Altinok and A. Bodek and A. Bravar and H. Budd and M. Bustamante and A. Butkevich and {Martinez Caicedo}, {D. A.} and Carneiro, {M. F.} and Castromonte, {C. M.} and Christy, {M. E.} and J. Chvojka and {Da Motta}, H. and M. Datta and J. Devan and Dytman, {S. A.} and D{\'i}az, {G. A.} and B. Eberly and J. Felix and L. Fields and R. Fine and Fiorentini, {G. A.} and A. Gago and H. Gallagher and R. Gran and Harris, {D. A.} and A. Higuera and K. Hurtado and J. Kleykamp and M. Kordosky and Kulagin, {S. A.} and T. Le and E. Maher and S. Manly and Mann, {W. A.} and Marshall, {C. M.} and {Martin Mari}, C. and McFarland, {K. S.} and McGivern, {C. L.} and McGowan, {A. M.} and B. Messerly and J. Miller and A. Mislivec and Morf{\'i}n, {J. G.} and J. Mousseau and T. Muhlbeier and D. Naples and Nelson, {J. K.} and A. Norrick and J. Osta and V. Paolone and J. Park and Patrick, {C. E.} and Perdue, {G. N.} and L. Rakotondravohitra and Ransome, {R. D.} and H. Ray and L. Ren and Rodrigues, {P. A.} and D. Ruterbories and H. Schellman and Schmitz, {D. W.} and C. Simon and Snider, {F. D.} and Sobczyk, {J. T.} and {Solano Salinas}, {C. J.} and N. Tagg and Tice, {B. G.} and E. Valencia and J. Wolcott and M. Wospakrik and G. Zavala and D. Zhang and Ziemer, {B. P.}",

year = "2015",

month = apr,

day = "1",

language = "Espa{\~n}ol",

volume = "91",

journal = "Physical Review D - Particles, Fields, Gravitation and Cosmology",

issn = "1550-7998",

}

Walton, T, Betancourt, M, Aliaga, L, Altinok, O, Bodek, A, Bravar, A, Budd, H, Bustamante, M, Butkevich, A, Martinez Caicedo, DA, Carneiro, MF, Castromonte, CM, Christy, ME, Chvojka, J, Da Motta, H, Datta, M, Devan, J, Dytman, SA, Díaz, GA, Eberly, B, Felix, J, Fields, L, Fine, R, Fiorentini, GA, Gago, A, 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, Martin Mari, C, McFarland, KS, McGivern, CL, McGowan, AM, Messerly, B, Miller, J, Mislivec, A, Morfín, 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, Solano Salinas, CJ, Tagg, N, Tice, BG, Valencia, E, Wolcott, J, Wospakrik, M, Zavala, G, Zhang, D & Ziemer, BP 2015, 'Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV', Physical Review D - Particles, Fields, Gravitation and Cosmology, vol. 91.

TY - JOUR

T1 - Measurement of muon plus proton final states in νμ interactions on hydrocarbon at Eν =4.2GeV

AU - Walton, T.

AU - Betancourt, M.

AU - Aliaga, L.

AU - Altinok, O.

AU - Bodek, A.

AU - Bravar, A.

AU - Budd, H.

AU - Bustamante, M.

AU - Butkevich, A.

AU - Martinez Caicedo, D. A.

AU - Carneiro, M. F.

AU - Castromonte, C. M.

AU - Christy, M. E.

AU - Chvojka, J.

AU - Da Motta, H.

AU - Datta, M.

AU - Devan, J.

AU - Dytman, S. A.

AU - Díaz, G. A.

AU - Eberly, B.

AU - Felix, J.

AU - Fields, L.

AU - Fine, R.

AU - Fiorentini, G. A.

AU - Gago, A.

AU - Gallagher, H.

AU - Gran, R.

AU - Harris, D. A.

AU - Higuera, A.

AU - Hurtado, K.

AU - Kleykamp, J.

AU - Kordosky, M.

AU - Kulagin, S. A.

AU - Le, T.

AU - Maher, E.

AU - Manly, S.

AU - Mann, W. A.

AU - Marshall, C. M.

AU - Martin Mari, C.

AU - McFarland, K. S.

AU - McGivern, C. L.

AU - McGowan, A. M.

AU - Messerly, B.

AU - Miller, J.

AU - Mislivec, A.

AU - Morfín, J. G.

AU - Mousseau, J.

AU - Muhlbeier, T.

AU - Naples, D.

AU - Nelson, J. K.

AU - Norrick, A.

AU - Osta, J.

AU - Paolone, V.

AU - Park, J.

AU - Patrick, C. E.

AU - Perdue, G. N.

AU - Rakotondravohitra, L.

AU - Ransome, R. D.

AU - Ray, H.

AU - Ren, L.

AU - Rodrigues, P. A.

AU - Ruterbories, D.

AU - Schellman, H.

AU - Schmitz, D. W.

AU - Simon, C.

AU - Snider, F. D.

AU - Sobczyk, J. T.

AU - Solano Salinas, C. J.

AU - Tagg, N.

AU - Tice, B. G.

AU - Valencia, E.

AU - Wolcott, J.

AU - Wospakrik, M.

AU - Zavala, G.

AU - Zhang, D.

AU - Ziemer, B. P.

PY - 2015/4/1

Y1 - 2015/4/1

N2 - 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° 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.

AB - 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° 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.

M3 - Artículo

SN - 1550-7998

VL - 91

JO - Physical Review D - Particles, Fields, Gravitation and Cosmology

JF - Physical Review D - Particles, Fields, Gravitation and Cosmology

ER -