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Beam Asymmetry Σ for the photoproduction of η and η mesons at Eγ=8.8 GeV

Abstract:

We report on the measurement of the beam asymmetry Σ for the reactions γppη and γppη from the GlueX experiment, using an 8.2-8.8 GeV linearly polarized tagged photon beam incident on a liquid hydrogen target in Hall D at Jefferson Lab. These measurements are made as a function of momentum transfer t, with significantly higher statistical precision than our earlier η measurements, and are the first measurements of η in this energy range. We compare the results to theoretical predictions based on t-channel quasi-particle exchange. We also compare the ratio of Ση to Ση to these models, as this ratio is predicted to be sensitive to the amount of sˉs exchange in the production. We find that photoproduction of both η and η is dominated by natural parity exchange with little dependence on t.

Journal: Phys. Rev. C100, 052201(R) (2019)

arXiv: arXiv:1908.05563

HEPdata: link


PRC 100, 052201(R) (2019): downloads png pdf
Figure 1:
The measured degree of linear polarization for the four diamond orientations is plotted as a function of the photon energy, offset from one another in energy for clarity. Events with energy between 8.2-8.8 GeV are selected, as demarcated by the vertical lines.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 2a:
The 2γ (a) and π+πη (b) invariant mass distributions are graphed after all selection cuts are applied. The η and η peak region samples consist of the events between the solid vertical lines. The “side-band region” samples include events between the vertical dashed lines and are used to evaluate the background asymmetry. The dashed curve on (a) is a MC calculation of the reaction γppω where the ωπ0γ and one of the resulting photons is not detected.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 3a:
The yields of η (a) and η (b) events are plotted as a function of t after all selection cuts are applied. The acceptance functions for γpηp(pγγ) and γpηp(pπ+πγγ), shown as the dashed curves, are determined from Monte Carlo simulation using a Regge model.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 3b:
The yields of η (a) and η (b) events are plotted as a function of t after all selection cuts are applied. The acceptance functions for γpηp(pγγ) and γpηp(pπ+πγγ), shown as the dashed curves, are determined from Monte Carlo simulation using a Regge model.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 4a:
(a) The yields integrated over the full range of t, Y and Y, are shown for the η events using one set of orthogonally polarized data, and (b) the yield asymmetry is shown, fitted with a χ2/ndf=25.59/28.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 4b:
(a) The yields integrated over the full range of t, Y and Y, are shown for the η events using one set of orthogonally polarized data, and (b) the yield asymmetry is shown, fitted with a χ2/ndf=25.59/28.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 5:
The photon beam asymmetry Ση is shown as a function of t for γppη. The vertical error bars represent the total errors and the horizontal error bars along with predictions for several Regge theory calculations. Previous GlueX (2017) results [13] are shown along with predictions for several Regge theory calculations, Laget [25,26], JPAC [3], EtaMAID [27], and Goldsein [28]. The 2.1% relative uncertainty is due largely to the polarization measurement.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 6:
The photon beam asymmetry Ση is shown for γppη. The vertical error bars represent the total errors and the horizontal error bars represent the RMS widths of the t distributions in each bin. The Regge theory calculation from JPAC [3] is shown.

PRC 100, 052201(R) (2019): downloads png pdf
Figure 7:
The photon beam asymmetry ratio Ση/Ση is plotted. The vertical error bars represent total errors. The horizontal error bars represent the RMS widths of the t distributions in each bin. The Regge theory calculation from JPAC [13] is shown.