28 research outputs found

    On transverse single-spin asymmetries in DD-meson production at the SPD NICA experiment

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    In the present study we are interested in the Sivers effect in process p↑pβ†’DXp^{\uparrow}p\to DX. We calculate the transverse single-spin asymmetry (TSSA) of DD-meson production within two phenomenological models, namely the Generalized Parton Model (GPM) and it's Colour Gauge-Invariant formulation (CGI-GPM), which takes into account the transverse momenta of initial partons. The last one allows us to study process-independent Sivers functions. To predict production cross-section of DD-mesons we use a fragmentation approach with scale-independent Peterson fragmentation function, taking in mind nonzero masses of cc-quark and DD-mesons. Estimates for the TSSAs, as a function of transverse momentum and Feynman variable xFx_F of DD-meson, within the conditions of the planned SPD NICA experiment are presented for the first time.Comment: 6 pages, 3 figures, Talk at the International Conference on Quantum Field Theory, High-Energy Physics, and Cosmology, 18-21 June 2022 BLTP, JIN

    Open charm production in the parton Reggeization approach: from Tevatron to LHC

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    We study the inclusive hadroproduction of D^0, D^+, D^star+, and D_s^+ mesons at leading order in the parton Reggeization approach endowed with universal fragmentation functions fitted to e+eβˆ’e^+e^- annihilation data from CERN LEP1. We have described DD-meson transverse momentum distributions measured in the central region of rapidity by the CDF Collaboration at Tevatron (|y|<1) and ALICE Collaboration at LHC (|y|<0.5) within uncertainties and without free parameters, using Kimber-Martin-Ryskin unintegrated gluon distribution function in a proton. The forward D-meson production (|y|>2.0) measured by the LHCb Collaboration also has been studied and expected disagreement between our theoretical predictions and data has been obtained.Comment: 16 pages, 12 figure

    B-meson production in the Parton Reggeization Approach at Tevatron and the LHC

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    We study the inclusive hadroproduction of B0B^0, B+B^+, and Bs0B_s^0 mesons at leading order in the parton Reggeization approach using the universal fragmentation functions extracted from the combined e+eβˆ’e^+e^- annihilation data from CERN LEP1 and SLAC SLC colliders. We have described BB-meson transverse momentum distributions measured in the central region of rapidity by the CDF Collaboration at Fermilab Tevatron and CMS Collaboration at LHC within uncertainties and without free parameters, applying Kimber-Martin-Ryskin unintegrated gluon distribution function in a proton. The forward BB-meson production (2.0<y<4.52.0<y<4.5) measured by the LHCb Collaboration also has been studied and expected disagreement between our theoretical predictions and data has been obtained.Comment: 17 pages, 11 figures. arXiv admin note: substantial text overlap with arXiv:1410.713

    Probing Gluons at the Spin Physics Detector

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    The Spin Physics Detector (SPD) at the Nuclotron based Ion Collider fAcility (NICA) is a multi-purpose experiment designed to study nucleon spin structure in the three dimensions. With capabilities to collide polarized protons and deuterons with center of mass energy up to 27 GeV and luminosity up to 1032cmβˆ’2Β sβˆ’110^{32} \rm cm^{-2} \ s^{-1} for protons (an order of magnitude less for deuterons), the experiment will allow measurements of cross-sections and spin asymmetries of hadronic processes sensitive to the unpolarized and various polarized (helicity, Sivers, Boer-Mulders) gluon distributions inside the nucleons. Results from the SPD will be complementary to the present high energy spin experiments at the RHIC facility or future experiments like the EIC (at BNL) and AFTER (at LHC). SPD will provide data in moderate and large Bjorken-x for much improved global analyses of spin structures of the basic building blocks of Nature. With polarized deuteron collisions, SPD will be the unique laboratory for probing tensor polarized gluon distributions. In addition, there are also possibilities of colliding other light nuclei like Carbon at reduced collision energy and luminosity at the first stage of the experiment.Comment: Accepted for publication in MDPI Physics special issue `From Heavy Ions to Astroparticle Physics
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