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Transition form factors: gamma* plus p -> Delta(1232), Delta(1600)

dc.contributor.authorLu, Y.
dc.contributor.authorChen, C. [UNESP]
dc.contributor.authorCui, Z-F
dc.contributor.authorRoberts, C. D.
dc.contributor.authorSchmidt, S. M.
dc.contributor.authorSegovia, J.
dc.contributor.authorZong, H-S
dc.contributor.institutionNanjing Univ
dc.contributor.institutionUniversidade Estadual Paulista (Unesp)
dc.contributor.institutionArgonne Natl Lab
dc.contributor.institutionForschungszentrum Julich
dc.contributor.institutionJARA
dc.contributor.institutionUniv Pablo Olavide
dc.contributor.institutionJoint Ctr Particle Nucl Phys & Cosmol
dc.contributor.institutionJustus Liebig Univ Giessen
dc.date.accessioned2019-10-04T12:40:23Z
dc.date.available2019-10-04T12:40:23Z
dc.date.issued2019-08-05
dc.description.abstractElectroproduction form factors describing the gamma* p -> Delta(+)(1232), Delta(+)(1600) transitions are computed using a fully dynamical diquark-quark approximation to the Poincare-covariant three-body bound-state problem in relativistic quantum field theory. In this approach, the Delta(1600) is an analogue of the Roper resonance in the nucleon sector, appearing as the simplest radial excitation of the Delta(1232). Precise measurements of the gamma* p -> Delta(+)(1232) transition already exist on 0 <= Q(2) less than or similar to 8 GeV2, and the calculated results compare favorably with the data outside the meson-cloud domain. The predictions for the gamma* p -> Delta(+)(1600) magnetic dipole and electric quadrupole transition form factors are consistent with the empirical values at the real photon point, and extend to Q(2) approximate to 6m(p)(2), enabling a meaningful direct comparison with experiment once analysis of existing data is completed. In both cases, the electric quadrupole form factor is particularly sensitive to deformation of the Delta-baryons. Interestingly, while the gamma* p -> Delta(+)(1232) transition form factors are larger in magnitude than those for gamma* p -> Delta(+)(1600) in some neighborhood of the real photon point, this ordering is reversed on Q(2) greater than or similar to 2m(p)(2), suggesting that the gamma* p -> Delta(+)(1600) transition is more localized in configuration space.en
dc.description.affiliationNanjing Univ, Dept Phys, Nanjing 210093, Jiangsu, Peoples R China
dc.description.affiliationUniv Estadual Paulista, Inst Fis Teor, Rua Dr Bento Teobaldo Ferraz 271, Sao Paulo, SP, Brazil
dc.description.affiliationArgonne Natl Lab, Phys Div, Lemont, IL 60439 USA
dc.description.affiliationForschungszentrum Julich, Inst Adv Simulat, D-52425 Julich, Germany
dc.description.affiliationJARA, D-52425 Julich, Germany
dc.description.affiliationUniv Pablo Olavide, Dept Sistemas Fis Quim & Nat, E-41013 Seville, Spain
dc.description.affiliationJoint Ctr Particle Nucl Phys & Cosmol, Nanjing 210093, Jiangsu, Peoples R China
dc.description.affiliationJustus Liebig Univ Giessen, Inst Theoret Phys, D-35392 Giessen, Germany
dc.description.affiliationUnespUniv Estadual Paulista, Inst Fis Teor, Rua Dr Bento Teobaldo Ferraz 271, Sao Paulo, SP, Brazil
dc.description.sponsorshipRWTH Aachen University, III. Physikalisches Institut B, Aachen-Germany
dc.description.sponsorshipUniversity of Huelva, Huelva-Spain
dc.description.sponsorshipUniversity of Pablo de Olavide, Seville-Spain, during the 4th Workshop on Nonperturbative QCD (University of Pablo de Olavide)
dc.description.sponsorshipNational Natural Science Foundation of China
dc.description.sponsorshipJiangsu Province Natural Science Foundation
dc.description.sponsorshipJiangsu Province Hundred Talents Plan for Professionals
dc.description.sponsorshipFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
dc.description.sponsorshipU.S. Department of Energy, Office of Science, Office of Nuclear Physics
dc.description.sponsorshipForschungszentrum Julich GmbH
dc.description.sponsorshipMinisterio de Economia Industria y Competitividad (MINECO)
dc.description.sponsorshipIdNational Natural Science Foundation of China: 11535005
dc.description.sponsorshipIdNational Natural Science Foundation of China: 11690030
dc.description.sponsorshipIdNational Natural Science Foundation of China: 11805097
dc.description.sponsorshipIdJiangsu Province Natural Science Foundation: BK20180323
dc.description.sponsorshipIdFAPESP: 2015/21550-4
dc.description.sponsorshipIdU.S. Department of Energy, Office of Science, Office of Nuclear Physics: DE-AC02-06CH11357
dc.description.sponsorshipIdMinisterio de Economia Industria y Competitividad (MINECO): FPA2017-86380-P
dc.format.extent13
dc.identifierhttp://dx.doi.org/10.1103/PhysRevD.100.034001
dc.identifier.citationPhysical Review D. College Pk: Amer Physical Soc, v. 100, n. 3, 13 p., 2019.
dc.identifier.doi10.1103/PhysRevD.100.034001
dc.identifier.issn2470-0010
dc.identifier.urihttp://hdl.handle.net/11449/185991
dc.identifier.wosWOS:000478997000002
dc.language.isoeng
dc.publisherAmer Physical Soc
dc.relation.ispartofPhysical Review D
dc.rights.accessRightsAcesso aberto
dc.sourceWeb of Science
dc.titleTransition form factors: gamma* plus p -> Delta(1232), Delta(1600)en
dc.typeArtigo
dcterms.licensehttp://publish.aps.org/authors/transfer-of-copyright-agreement
dcterms.rightsHolderAmer Physical Soc
dspace.entity.typePublication
unesp.campusUniversidade Estadual Paulista (UNESP), Instituto de Física Teórica (IFT), São Paulopt

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