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Nuclear shadowing in photoproduction of rho mesons in ultraperipheral nucleus collisions at RHIC and the LHC

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arxiv 1506.07150 v2 pith:IUHFPG5U submitted 2015-06-23 hep-ph hep-exnucl-ex

Nuclear shadowing in photoproduction of rho mesons in ultraperipheral nucleus collisions at RHIC and the LHC

classification hep-ph hep-exnucl-ex
keywords crossnuclearphotoproductionsectionshadowinginelasticelasticenergy
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We argue that with an increase of the collision energy, elastic photoproduction of $\rho$ mesons on nuclei becomes affected by the significant cross section of photon inelastic diffraction into large masses, which results in the sizable inelastic nuclear shadowing correction to $\sigma_{\gamma A \to \rho A}$ and the reduced effective $\rho$-nucleon cross section. We take these effects into account by combining the vector meson dominance model, which we upgrade to include the contribution of high-mass fluctuations of the photon according to QCD constraints, and the Gribov-Glauber approximation for nuclear shadowing, where the inelastic nuclear shadowing is included by means of cross section fluctuations. The resulting approach allows us to successfully describe the data on elastic $\rho$ photoproduction on nuclei in heavy ion UPCs in the $7 \ {\rm GeV} < W_{\gamma p} < 46$ GeV energy range and to predict the value of the cross section of coherent $\rho$ photoproduction in Pb-Pb UPCs at $\sqrt{s_{NN}}=5.02$ TeV in Run 2 at the LHC, $d\sigma_{Pb Pb \to \rho Pb Pb} (y=0)/dy= 560 \pm 25$ mb.

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  1. Coherent photoproduction of light vector mesons off nuclear targets in the dipole picture

    hep-ph 2023-10 unverdicted novelty 3.0

    A suppression factor R_G=0.85 is tuned to F2 and rho photoproduction data and used to predict observables for rho(2S), omega, and phi states via holographic wave functions in the dipole picture.