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Exclusive <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi></mml:mrow><mml:mo>,</mml:mo><mml:mo> </mml:mo><mml:mrow><mml:mi>ψ</mml:mi><mml:mo>(</mml:mo><mml:mn>2</mml:mn><mml:mi>s</mml:mi><mml:mo>)</mml:mo></mml:mrow></mml:math>, and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msup><mml:mi>e</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:msup><mml:mi>e</mml:mi><mml:mo>−</mml:mo></mml:msup></mml:mrow></mml:math> pair production in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>Au</mml:mi><mml:mo>+</mml:mo><mml:mi>Au</mml:mi></mml:mrow></mml:math> ultraperipheral collisions at the BNL Relativistic Heavy Ion Collider

M. I. AbdulhamidAmerican University in CairoB. E. AboonaTexas A&M UniversityJ. AdamCzech Technical University in PragueL. AdamczykAGH University of KrakowJ. R. AdamsThe Ohio State UniversityY. HuPanjab UniversityM. M. AggarwalPanjab UniversityZ. AhammedVariable Energy Cyclotron CentreE. C. AschenauerBrookhaven National LaboratorySaba AslamIndian Institute TechnologyJ. AtchisonAbilene Christian UniversityV. BairathiJ. BallUniversity of HoustonK. N. BarishUniversity of CaliforniaR. BellwiedUniversity of HoustonP. BhagatUniversity of JammuA. BhasinUniversity of JammuS. BhattaState University of New YorkS. R. BhosaleELTE Eötvös Loránd UniversityJ. BielcikCzech Technical University in PragueJ. BielcikovaNuclear Physics Institute of the CASJ. D. BrandenburgThe Ohio State UniversityC. BroodoUniversity of HoustonX. Z. CaiShanghai Institute of Applied PhysicsH. CainesYale UniversityM. Calderon De La Barca SanchezUniversity of CaliforniaD. CebraUniversity of CaliforniaJ. CeskaCzech Technical University in PragueI. ChakaberiaLawrence Berkeley National LaboratoryP. ChaloupkaCzech Technical University in PragueB. K. ChanUniversity of CaliforniaZ. ChangIndiana UniversityA. ChatterjeeNational Institute of Technology DurgapurD. ChenUniversity of CaliforniaJ. ChenFudan UniversityJ. H. ChenFudan UniversityZ. ChenShandong UniversityJ. ChengTsinghua UniversityY. ChengUniversity of CaliforniaS. ChoudhuryFudan UniversityW. ChristieBrookhaven National LaboratoryX. ChuBrookhaven National LaboratoryH. J. CrawfordUniversity of CaliforniaM. CsanádELTE Eötvös Loránd UniversityG. Dale-GauUniversity of Illinois at ChicagoArkaprava DasCzech Technical University in PragueI. M. DeppnerUniversity of HeidelbergA. DhamijaPanjab UniversityP. DixitIndian Institute of Science Education and Research (IISER)X. DongLawrence Berkeley National LaboratoryJ. L. DrachenbergAbilene Christian UniversityE. DuckworthKent State UniversityJ. C. DunlopBrookhaven National LaboratoryJ. EngelageUniversity of CaliforniaG. EppleyRice UniversityS. EsumiUniversity of TsukubaO. EvdokimovUniversity of Illinois at ChicagoO. EyserBrookhaven National LaboratoryR. FatemiUniversity of KentuckyS. FazioUniversity of Calabria & INFN-CosenzaC. FengNational Cheng Kung UniversityY. FengPurdue UniversityE. FinchSouthern Connecticut State UniversityY. FisyakBrookhaven National LaboratoryF. FlorYale UniversityC. FuInstitute of Modern PhysicsC. A. GagliardiTexas A&M UniversityT. GalatyukTechnische Universität DarmstadtTong GaoShandong UniversityF. J. M. GeurtsRice UniversityN. GhimireTemple UniversityS. M. GibsonValparaiso UniversityK. GopalIndian Institute of Science Education and Research (IISER) TirupatiX. GouShandong UniversityD. GrosnickValparaiso UniversityA. GuptaUniversity of JammuW. GurynBrookhaven National LaboratoryA. HamedAmerican University in CairoY. F. HanRice UniversityS. HarabaszTechnische Universität DarmstadtM. D. HarastyUniversity of CaliforniaJ. W. HarrisYale UniversityH. Harrison-SmithUniversity of KentuckyWei HeFudan UniversityX. H. HeInstitute of Modern PhysicsY. HeShandong UniversityN. HerrmannUniversity of HeidelbergL. HolubCzech Technical University in PragueC. HuUniversity of Chinese Academy of SciencesQ. HuInstitute of Modern PhysicsH. Z. HuangNational Cheng Kung UniversityS. HuangState University of New YorkTao HuangUniversity of Illinois at ChicagoX. HuangTsinghua UniversityY. HuangCentral China Normal UniversityT. J. HumanicThe Ohio State UniversityM. IsshikiUniversity of Tsukuba
Physical review. Cjournal2024lv
ABI

Аннотация

Measurements of exclusive $J/\ensuremath{\psi}, \ensuremath{\psi}(2s)$, and electron-positron (${e}^{+}{e}^{\ensuremath{-}}$) pair photoproduction in $\mathrm{Au}+\mathrm{Au}$ ultraperipheral collisions are reported by the STAR experiment at $\sqrt{{s}_{{}_{\mathrm{NN}}}}=200\phantom{\rule{4pt}{0ex}}\mathrm{GeV}$. We report several first measurements at the BNL Relativistic Heavy Ion Collider, which are (i) $J/\ensuremath{\psi}$ photoproduction with large momentum transfer up to ${2.2\phantom{\rule{4pt}{0ex}}(\mathrm{GeV}/c)}^{2}$, (ii) coherent $J/\ensuremath{\psi}$ photoproduction associated with neutron emissions from nuclear breakup, (iii) the rapidity dependence of incoherent $J/\ensuremath{\psi}$ photoproduction, (iv) the $\ensuremath{\psi}(2s)$ photoproduction cross section at midrapidity, and (v) ${e}^{+}{e}^{\ensuremath{-}}$ pair photoproduction up to high invariant mass of $6\phantom{\rule{4pt}{0ex}}\mathrm{GeV}/{c}^{2}$. For measurement (ii), the coherent $J/\ensuremath{\psi}$ total cross section of $\ensuremath{\gamma}+\mathrm{Au}\ensuremath{\rightarrow}\mathrm{J}/\ensuremath{\psi}+\mathrm{Au}$ as a function of the center-of-mass energy ${W}_{\ensuremath{\gamma}N}$ has been obtained without photon energy ambiguities. The data are quantitatively compared with the Monte Carlo models STARlight, Sartre, BeAGLE, and theoretical calculations of gluon saturation with color glass condensate, nuclear shadowing with leading twist approximation, quantum electrodynamics, and the next-to-leading-order perturbative QCD. At the photon-nucleon center-of-mass energy of 25.0 GeV, the coherent and incoherent $J/\ensuremath{\psi}$ cross sections of Au nuclei are found to be $71%\ifmmode\pm\else\textpm\fi{}10%$ and $36%\ifmmode\pm\else\textpm\fi{}7%$, respectively, of that of free protons. These data provide an important experimental constraint for nuclear parton distribution functions and a unique opportunity to advance the understanding of the nuclear modification effect at the top RHIC energy.

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