The exclusive photoproduction reactions γp → J/ψ(1S)p and γp → ψ(2S)p have been measured at an ep centre-of-mass energy of 318 GeV with the ZEUS detector at HERA using an integrated luminosity of 373 pb −1. The measurement was made in the kinematic range 30 < W < 180 GeV, Q 2 < 1 GeV2 and |t| < 1 GeV2, where W is the photon-proton centre-of-mass energy, Q 2 is the photon virtuality and t is the squared four-momentum transfer at the proton vertex. The decay channels used were J/ψ(1S) → μ + μ − , ψ(2S) → μ + μ − and ψ(2S) → J/ψ(1S)π + π − with subsequent decay J/ψ(1S) → μ + μ − . The ratio of the production cross sections, R = σ ψ(2S) /σ J/ψ(1S), has been measured as a function of W and |t| and compared to previous data in photoproduction and deep inelastic scattering and with predictions of QCD-inspired models of exclusive vector-meson production, which are in reasonable agreement with the data.
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London, London, United Kingdom", "organization": "University College London" } ], "surname": "Wing", "email": "m.wing@ucl.ac.uk", "full_name": "Wing, M.", "given_names": "M." }, { "affiliations": [ { "country": "Japan", "value": "Institute of Particle and Nuclear Studies, KEK, Tsukuba, Japan", "organization": "Institute of Particle and Nuclear Studies, KEK" } ], "surname": "Yamada", "given_names": "S.", "full_name": "Yamada, S." }, { "affiliations": [ { "country": "Japan", "value": "Department of Physics, Kobe University, Kobe, Japan", "organization": "Kobe University" } ], "surname": "Yamazaki", "given_names": "Y.", "full_name": "Yamazaki, Y." }, { "affiliations": [ { "country": "Poland", "value": "Faculty of Physics, University of Warsaw, Warsaw, Poland", "organization": "University of Warsaw" } ], "surname": "\u017barnecki", "given_names": "A.", "full_name": "\u017barnecki, A." }, { "affiliations": [ { "country": "Germany", "value": "Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany", "organization": "Deutsches Elektronen-Synchrotron DESY" }, { "country": "CERN", "value": "CERN, Geneva, Switzerland", "organization": "CERN" } ], "surname": "Zenaiev", "given_names": "O.", "full_name": "Zenaiev, O." } ], "titles": [ { "source": "Springer", "title": "Measurement of the cross-section ratio \u03c3 \u03c8(2S) /\u03c3 J/\u03c8(1S) in exclusive photoproduction at HERA" } ], "dois": [ { "value": "10.1007/JHEP12(2022)164" } ], "publication_info": [ { "page_end": "27", "journal_title": "Journal of High Energy Physics", "material": "article", "journal_volume": "2022", "artid": "JHEP12(2022)164", "year": 2022, "page_start": "1", "journal_issue": "12" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2023-03-26T00:31:17.262657", "source": "Springer", "method": "Springer", "submission_number": "57ba2b5ecb6d11eda920065bd8dc6b20" }, "page_nr": [ 27 ], "license": [ { "url": "https://creativecommons.org/licenses//by/4.0", "license": "CC-BY-4.0" } ], "copyright": [ { "holder": "The Author(s)", "year": "2022" } ], "control_number": "74853", "collaborations": [ { "value": "The ZEUS collaboration" } ], "_files": [ { "checksum": "md5:685cc21b13bbbd9a6358102a5d1670f8", "filetype": "xml", "bucket": "109c1abe-a675-4f05-89ab-d856df3f7c39", "version_id": "3ef04a1d-dad4-46d2-915d-0da17ec77074", "key": "10.1007/JHEP12(2022)164.xml", "size": 65462 }, { "checksum": "md5:92d96502a1343d66000ad41898a12804", "filetype": "pdf/a", "bucket": "109c1abe-a675-4f05-89ab-d856df3f7c39", "version_id": "88d97615-9e0e-40e3-93e7-69296008a2bb", "key": "10.1007/JHEP12(2022)164_a.pdf", "size": 974628 } ], "record_creation_date": "2022-12-31T03:30:23.190269", "collections": [ { "primary": "Journal of High Energy Physics" } ], "arxiv_eprints": [ { "categories": [ "hep-ex", "hep-ph" ], "value": "2206.13343" } ], "abstracts": [ { "source": "Springer", "value": "The exclusive photoproduction reactions \u03b3p \u2192 J/\u03c8(1S)p and \u03b3p \u2192 \u03c8(2S)p have been measured at an ep centre-of-mass energy of 318 GeV with the ZEUS detector at HERA using an integrated luminosity of 373 pb \u22121. The measurement was made in the kinematic range 30 < W < 180 GeV, Q 2 < 1 GeV2 and |t| < 1 GeV2, where W is the photon-proton centre-of-mass energy, Q 2 is the photon virtuality and t is the squared four-momentum transfer at the proton vertex. The decay channels used were J/\u03c8(1S) \u2192 \u03bc + \u03bc \u2212 , \u03c8(2S) \u2192 \u03bc + \u03bc \u2212 and \u03c8(2S) \u2192 J/\u03c8(1S)\u03c0 + \u03c0 \u2212 with subsequent decay J/\u03c8(1S) \u2192 \u03bc + \u03bc \u2212 . The ratio of the production cross sections, R = \u03c3 \u03c8(2S) /\u03c3 J/\u03c8(1S), has been measured as a function of W and |t| and compared to previous data in photoproduction and deep inelastic scattering and with predictions of QCD-inspired models of exclusive vector-meson production, which are in reasonable agreement with the data." } ], "imprints": [ { "date": "2022-12-29", "publisher": "Springer" } ] }