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Transverse single-spin asymmetry in the low-virtuality leptoproduction of open charm as a probe of the gluon Sivers function

Rohini M. Godbole, Abhiram Kaushik, and Anuradha Misra
Phys. Rev. D 97, 076001 – Published 4 April 2018

Abstract

We study the low-virtuality inclusive leptoproduction of open charm, plD0+X as a probe of the gluon Sivers function. We perform the analysis in a generalized parton model framework. At leading order, this process is sensitive only to the gluon content of the proton. Hence any detection of a transverse single-spin asymmetry in this process would be clear indication of a non-zero gluon Sivers function (GSF). Considering COMPASS and a future Electron-Ion Collider (EIC), we present predictions for asymmetry using fits for the GSF available in literature. Predictions for peak asymmetry values lie in the range of 0.8% to 13%. We also present estimates of the upper bound on the asymmetry as obtained with a maximal gluon Sivers function. Further, for the case of the Electron-Ion Collider, we evaluate the asymmetry in the muons decaying from the D-meson and find that the asymmetry is well preserved in the kinematics of the muons. Peak values of the muon asymmetry are close to those obtained for the D-meson and lie in the range 0.75% to 11%.

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  • Received 18 December 2017

DOI:https://doi.org/10.1103/PhysRevD.97.076001

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Particles & Fields

Authors & Affiliations

Rohini M. Godbole1,*, Abhiram Kaushik1,†, and Anuradha Misra2,‡

  • 1Centre for High Energy Physics, Indian Institute of Science, Bangalore 560012, India
  • 2Department of Physics, University of Mumbai, Mumbai 400098, India

  • *rohini@chep.iisc.ernet.in
  • abhiramb@chep.iisc.ernet.in
  • misra@physics.mu.ac.in

Article Text

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Issue

Vol. 97, Iss. 7 — 1 April 2018

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Images

  • Figure 1
    Figure 1

    Kinematics for COMPASS (left) and EIC (right). PN is the proton momentum and S is its spin orientation. Pl is the lepton momentum. The D-meson momentum, PD is taken to be on the xz plane.

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  • Figure 2
    Figure 2

    Unpolarized cross section at COMPASS as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 3
    Figure 3

    SSA with saturated GSF at COMPASS as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 4
    Figure 4

    SSA from GSF fits of Ref. [9] at COMPASS as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 5
    Figure 5

    Unpolarized cross section at EIC as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 6
    Figure 6

    SSA with saturated GSF at EIC as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 7
    Figure 7

    SSA from GSF fits of Ref. [9] at EIC as a function of xF (at fixed PT, left panel) and PT (at fixed η, right panel).

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  • Figure 8
    Figure 8

    Cross section (left panel) and SSA (right panel) for decay-muons.

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