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  • Open Access

First Measurement of Hard Exclusive πΔ++ Electroproduction Beam-Spin Asymmetries off the Proton

S. Diehl et al. (CLAS Collaboration)
Phys. Rev. Lett. 131, 021901 – Published 11 July 2023
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Abstract

The polarized cross-section ratio σLT/σ0 from hard exclusive πΔ++ electroproduction off an unpolarized hydrogen target has been extracted based on beam-spin asymmetry measurements using a 10.2GeV/10.6GeV incident electron beam and the CLAS12 spectrometer at Jefferson Lab. The study, which provides the first observation of this channel in the deep-inelastic regime, focuses on very forward-pion kinematics in the valence regime, and photon virtualities ranging from 1.5GeV2 up to 7GeV2. The reaction provides a novel access to the d-quark content of the nucleon and to pΔ++ transition generalized parton distributions. A comparison to existing results for hard exclusive π+n and π0p electroproduction is provided, which shows a clear impact of the excitation mechanism, encoded in transition generalized parton distributions, on the asymmetry.

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  • Received 21 March 2023
  • Revised 22 May 2023
  • Accepted 20 June 2023

DOI:https://doi.org/10.1103/PhysRevLett.131.021901

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)

Nuclear Physics

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Article Text

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Issue

Vol. 131, Iss. 2 — 14 July 2023

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Images

  • Figure 1
    Figure 1

    Hard exclusive πΔ++ electroproduction off the proton in very forward kinematics (t/Q21) with the virtuality Q2 and the four-momentum transfer t to the Δ++.

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  • Figure 2
    Figure 2

    Upper row: Δ++ peak in the pπ+ invariant mass of the experimental data (blue, solid line) in comparison to the nonresonant background obtained with the SIDIS MC (black, dashed) for selected bins of t in the forward region (Q2=2.48GeV2, xB=0.27) after a cut on Mπ+π>1.1GeV. Lower row: Δ++ peak in the same bins after the subtraction of the background (blue, solid line) in comparison to the result from the exclusive MC (red, dashed line).

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  • Figure 3
    Figure 3

    Distribution of Q2 versus xB for t<1.5GeV2. The bin boundaries are shown as red lines (bin 1: xB<0.23; bin 2: xB>0.23, Q2<2.6GeV2; bin 3: xB>0.23, Q2>2.6GeV2).

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  • Figure 4
    Figure 4

    BSA as a function of ϕ for representative t bins (Q2=2.48GeV2, xB=0.27). The red line shows the sinϕ fit.

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  • Figure 5
    Figure 5

    σLT/σ0 and its statistical uncertainty for πΔ++ (black squares, this Letter) as a function of t=(|t||tmin|) in the forward kinematic regime and its systematic uncertainty (gray band). The subfigures correspond to the results for the different Q2 and xB bins defined in Fig. 3. The mean kinematics are shown on top of each subfigure. The corresponding result tables can be found in the Supplemental Material [25] and can be downloaded from Ref. [33]. For comparison, the results from the hard exclusive π+n (red triangles, Ref. [31]) and π0p (blue circles, Ref. [32]) electroproduction with similar kinematics are shown.

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