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A. C. Wang

Publications and source records attributed to A. C. Wang.

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Effects of $Δ(1905)5/2^+$ on $K^*Σ$ photoproduction

The two-channel photoproductions of $γp \to K^{*+} Σ^{0}$ and $γp \to K^{*0} Σ^{+}$ are investigated based on an effective Lagrangian approach at the tree-level Born approximation. In addition to the $t$-channel $K$, $κ$, $K^*$ exchanges, the $s$-channel nucleon ($N$) and $Δ$ exchanges, the $u$-channel $Λ$, $Σ$, $Σ^*$ exchanges, and the generalized contact term, we try to take into account the minimum number of baryon resonances in constructing the reaction amplitudes to describe the experimental data. It is found that by including the $Δ(1905)5/2^+$ resonance with its mass, width, and helicity amplitudes taken from the Review of Particle Physics [Particle Data Group, C. Patrignani {\it et al.}, Chin. Phys. C {\bf 40}, 100001 (2016)], the calculated differential and total cross sections for these two reactions are in good agreement with the experimental data. An analysis of the reaction mechanisms shows that the cross sections of $γp \to K^{*+}Σ^{0}$ are dominated by the $s$-channel $Δ(1905)5/2^+$ exchange at low energies and $t$-channel $K^*$ exchange at high energies, with the $s$-channel $Δ$ exchange providing significant contributions in the near-threshold region. For $γp \to K^{*0}Σ^{+}$, the angular dependences are dominated by the $t$-channel $K$ exchange at forward angles and the $u$-channel $Σ^*$ exchange at backward angles, with the $s$-channel $Δ$ and $Δ(1905)5/2^+$ exchanges making considerable contributions at low energies. Predictions are given for the beam, target, and recoil asymmetries for both reactions.

nucl-th

Nucleon resonances in $γp \to K^{*+} Λ$

The high-precision cross-section data for the reaction $γp \to K^{*+}Λ$ reported by the CLAS Collaboration at the Thomas Jefferson National Accelerator Facility have been analyzed based on an effective Lagrangian approach in the tree-level approximation. Apart from the $t$-channel $K$, $κ$, $K^*$ exchanges, the $s$-channel nucleon ($N$) exchange, the $u$-channel $Λ$, $Σ$, $Σ^*(1385)$ exchanges, and the generalized contact term, the contributions from the near-threshold nucleon resonances in the $s$-channel are also taken into account in constructing the reaction amplitude. It is found that, to achieve a satisfactory description of the differential cross section data, at least two nucleon resonances should be included. By including the $N(2060){5/2}^-$ resonance, which is responsible for the shape of the angular distribution near the $K^*Λ$ threshold, and one of the $N(2000){5/2}^+$, $N(2040){3/2}^+$, $N(2100){1/2}^+$, $N(2120){3/2}^-$ and $N(2190){7/2}^-$ resonances, one can describe the cross-section data quite well, with the fitted resonance masses and widths compatible with those advocated by the Particle Data Group. The resulted predictions of the beam, target, and recoil asymmetries are found to be quite different from various fits, indicating the necessity of the spin observable data for $γp \to K^{*+}Λ$ to further pin down the resonance contents and associated parameters in this reaction.

hep-ph