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dc.contributor.authorSirunyan, A. M
dc.contributor.authorTumasyan, A.
dc.contributor.authorAdam, W.
dc.contributor.authorAmbrogi, F.
dc.contributor.authorAsilar, E.
dc.contributor.authorBergauer, T.
dc.contributor.authorBrandstetter, J.
dc.contributor.authorDragicevic, M.
dc.contributor.authorErö, J.
dc.contributor.authorDel Valle, A. E
dc.contributor.authorFlechl, M.
dc.contributor.authorFrühwirth, R.
dc.contributor.authorGhete, V. M
dc.contributor.authorHrubec, J.
dc.contributor.authorJeitler, M.
dc.contributor.authorKrammer, N.
dc.contributor.authorKrätschmer, I.
dc.contributor.authorLiko, D.
dc.contributor.authorMadlener, T.
dc.contributor.authorMikulec, I.
dc.date.accessioned2021-09-20T17:28:59Z
dc.date.available2021-09-20T17:28:59Z
dc.date.issued2019-08-21
dc.identifier.urihttps://hdl.handle.net/1721.1/131616
dc.description.abstractAbstract Exclusive $${{{\uprho _{}^{}} _{}^{}}{{\left( {770}\right) }{}_{}^{}}} ^{0}$$ ρ 770 0 photoproduction is measured for the first time in ultraperipheral pPb collisions at $$\sqrt{\smash [b]{s_{_{\mathrm {NN}}}}} = 5.02\,\text {Te}\text {V} $$ s NN = 5.02 Te with the CMS detector. The cross section $$\sigma ({\upgamma _{}^{}} \mathrm{p}\rightarrow {{{\uprho _{}^{}} _{}^{}}{{\left( {770}\right) }{}_{}^{}}} ^{0}\mathrm{p})$$ σ ( γ p → ρ 770 0 p ) is $$11.0 \pm 1.4\,\text {(stat)} \pm 1.0\,\text {(syst)} $$ 11.0 ± 1.4 (stat) ± 1.0 (syst) $$\mu $$ μ b at $$\langle W_{{\upgamma _{}^{}} \mathrm{p}}\rangle = 92.6\,\text {Ge}\text {V} $$ ⟨ W γ p ⟩ = 92.6 Ge for photon–proton centre-of-mass energies $$W_{{\upgamma _{}^{}} \mathrm{p}}$$ W γ p between 29 and $$213\,\text {Ge}\text {V} $$ 213 Ge . The differential cross section $$\mathrm {d}\sigma /\mathrm {d}|t |$$ d σ / d | t | is measured in the interval $$0.025< |t | < 1\,\text {Ge}\text {V} ^{2}$$ 0.025 < | t | < 1 Ge 2 as a function of $$W_{{\upgamma _{}^{}} \mathrm{p}}$$ W γ p , where t is the squared four-momentum transfer at the proton vertex. The results are compared with previous measurements and theoretical predictions. The measured cross section $$\sigma ({\upgamma _{}^{}} \mathrm{p}\rightarrow {{{\uprho _{}^{}} _{}^{}}{{\left( {770}\right) }{}_{}^{}}} ^{0}\mathrm{p})$$ σ ( γ p → ρ 770 0 p ) has a power-law dependence on the photon–proton centre-of-mass, consistent with electron–proton collision measurements performed at HERA. The $$W_{{\upgamma _{}^{}} \mathrm{p}}$$ W γ p dependence of the exponential slope of the differential cross section $$\mathrm {d}\sigma /\mathrm {d}|t |$$ d σ / d | t | is also measured.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1140/epjc/s10052-019-7202-9en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleMeasurement of exclusive $${{{\uprho _{}^{}} _{}^{}}{{\left( {770}\right) }{}_{}^{}}} ^{0}$$ ρ 770 0  photoproduction in ultraperipheral pPb collisions at $$\sqrt{\smash [b]{s_{_{\mathrm {NN}}}}} = 5.02\,\text {Te}\text {V} $$ s NN = 5.02 Teen_US
dc.typeArticleen_US
dc.identifier.citationThe European Physical Journal C. 2019 Aug 21;79(8):702en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2020-06-26T12:42:05Z
dc.language.rfc3066en
dc.rights.holderCERN for the benefit of the CMS collaboration
dspace.embargo.termsN
dspace.date.submission2020-06-26T12:42:05Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Needed


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