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Beam Spin Asymmetry in Semi-Inclusive Electroproduction of Hadron Pairs

M. Mirazita et al. (CLAS Collaboration)
Phys. Rev. Lett. 126, 062002 – Published 12 February 2021
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Abstract

A first measurement of the longitudinal beam spin asymmetry ALU in the semi-inclusive electroproduction of pairs of charged pions is reported. ALU is a higher-twist observable and offers the cleanest access to the nucleon twist-3 parton distribution function e(x). Data have been collected in the Hall-B at Jefferson Lab by impinging a 5.498-GeV electron beam on a liquid-hydrogen target, and reconstructing the scattered electron and the pion pair with the CLAS detector. One-dimensional projections of the ALUsinϕR moments are extracted for the kinematic variables of interest in the valence quark region. The understanding of dihadron production is essential for the interpretation of observables in single-hadron production in semi-inclusive DIS, and pioneering measurements of single-spin asymmetries in dihadron production open a new avenue in studies of QCD dynamics.

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  • Received 26 October 2020
  • Revised 23 December 2020
  • Accepted 12 January 2021

DOI:https://doi.org/10.1103/PhysRevLett.126.062002

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 & FieldsAccelerators & BeamsNuclear Physics

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Issue

Vol. 126, Iss. 6 — 12 February 2021

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Images

  • Figure 1
    Figure 1

    BSA as a function of ϕR in the 6Δϕ bins from 180° to 180° for the bin x=0.2÷0.3. The full circles represent the experimental measurement with the vertical bar indicating the total uncertainty, while the curves represent the result of the fit with Eq. (8).

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  • Figure 2
    Figure 2

    Dependence on x (left) and Q2 (right) of the sinϕR moment ALUsinϕR of the BSA. The error bars and the gray band represents the statistical and systematic uncertainties.

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  • Figure 3
    Figure 3

    Dependence on z (left) and mππ (right) of the sinϕR moment ALUsinϕR of the BSA. The error bars and the gray band represents the statistical and systematic uncertainties.

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  • Figure 4
    Figure 4

    Dependence on x of the sinϕR moment ALUsinϕR of the beam-spin asymmetry compared to model calculations: the spectator model [26] in the green-dashed band, the bag model [27] in the red-full band, and the gray-dotted band corresponds to the LFCQM [24], all use the dihadron FFs [19].

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