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Measurement of the photon beam asymmetry in γpK+Σ0 at Eγ=8.5 GeV

S. Adhikari et al. (GlueX Collaboration )
Phys. Rev. C 101, 065206 – Published 25 June 2020

Abstract

We report measurements of the photon beam asymmetry Σ for the reaction γpK+Σ0(1193) using the GlueX spectrometer in Hall D at Jefferson Lab. Data were collected by using a linearly polarized photon beam in the energy range of 8.2–8.8 GeV incident on a liquid hydrogen target. The beam asymmetry Σ was measured as a function of the Mandelstam variable t, and a single value of Σ was extracted for events produced in the u channel. These are the first exclusive measurements of the photon beam asymmetry Σ for the reaction in this energy range. For the t channel, the measured beam asymmetry is close to unity over the t range studied, t=(0.11.4)(GeV/c)2, with an average value of Σ=1.00±0.05. This agrees with theoretical models that describe the reaction via the natural-parity exchange of the K*(892) Regge trajectory. A value of Σ=0.41±0.09 is obtained for the u channel integrated up to u=2.0 (GeV/c)2.

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  • Received 18 March 2020
  • Revised 21 April 2020
  • Accepted 11 May 2020

DOI:https://doi.org/10.1103/PhysRevC.101.065206

©2020 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

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Vol. 101, Iss. 6 — June 2020

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Images

  • Figure 1
    Figure 1

    Photon beam polarization as a function of beam energy, as measured by the triplet polarimeter, averaged over the four different diamond orientations. Dashed vertical lines indicate the beam-energy range used for this analysis. Vertical error bars show the statistical uncertainty and inner shaded regions show the systematic uncertainty due to the 1.5% relative uncertainty from the polarimeter analyzing power. The polarizations for the individual orientations are presented in Ref. [21].

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  • Figure 2
    Figure 2

    Invariant mass of pπγ vs invariant mass of pπ after all cuts. The enhancement in the overlap region corresponds to the Λ0(1116) and Σ0(1193).

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  • Figure 3
    Figure 3

    Invariant mass of pπ (solid circles). The solid curve is the sum of a Voigtian and a first-order Chebyshev polynomial (dashed curve) fit to the data. The selection region of Λ signal events is indicated by the vertical dashed lines.

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  • Figure 4
    Figure 4

    The invariant mass of Λγ (solid circles). The solid curve is the sum of a Voigtian and a first-order Chebyshev polynomial (dashed curve) fit to the data. The selection region of Σ0 events for further analysis is indicated by the vertical dashed lines.

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  • Figure 5
    Figure 5

    Event yields for γpK+Σ0 (solid circles) and detector acceptance (dashed lines) (a) as a function of t and (b) as a function of u.

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  • Figure 6
    Figure 6

    Yield of γpK+Σ0 events versus ϕ integrated over t for the 90 (open upward triangles) and 0 (solid downward triangles) polarization orientations.

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  • Figure 7
    Figure 7

    Yield of γpK+Σ0 events versus ϕ integrated over t for the 45 (open upward triangles) and 45 (solid downward triangles) polarization orientations.

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  • Figure 8
    Figure 8

    The yield asymmetry for the 0/90 orientation set, corresponding to the data in Fig. 6 with a fit of Eq. (9) (solid curve). See text for details.

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  • Figure 9
    Figure 9

    The yield asymmetry for the 45/45 orientation set, corresponding to the data in Fig. 7 with a fit of Eq. (9) (solid curve). See text for details.

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  • Figure 10
    Figure 10

    The beam asymmetry Σ for γpK+Σ0 as a function of t. The results from the 0/90 and 45/45 data sets are averaged (solid circles) where horizontal error bars indicate the rms widths of the t bins and vertical error bars represent statistical and systematic uncertainties added in quadrature. An additional 2.1% overall relative polarization uncertainty is not included. The triangles are previous SLAC results [2] at Eγ=16 GeV, the curves show predictions from RPR-2007 [6, 7] (solid) and Guidal et al. [5] (dashed) at Eγ=8.5 GeV.

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