June 27, 2022 to July 1, 2022
Prague, Czech Republic
Europe/Zurich timezone

The study of πΣ photoproduction in the Λ*(1405) region

Jun 27, 2022, 5:40 PM
15m
Hotel Pyramida

Hotel Pyramida

talk 1; Mon-IV

Speaker

Ales Cieply (Nuclear Physics Institute, Rez, Czechia)

Description

The measurements of $\pi\Sigma$ mass distributions in the $\gamma p \longrightarrow K^{+} \pi\Sigma$ photoproduction reaction [1, 2] probe the energy region of the $\Lambda(1405)$ resonance, just below the $\bar{K}N$ threshold, and present new challenges for the theoretical models of $\bar{K}N-\pi\Sigma$ coupled channels interactions. Adopting the model presented in [3] we describe the photoproduction reaction in terms of tree level amplitudes followed by the meson-baryon rescattering in the final state. For the latter we employ the $MB \longrightarrow \pi\Sigma$ amplitudes generated by our recent $\bar{K}N$ model [4]. Although our approach is similar to the one used earlier in [5], we use a different way to unitarize the photoproduction amplitude and avoid some non-relativistic approximations adopted in [5].

Our preliminary results show that the tree level photoproduction graphs (Weinberg-Tomozawa, Born and anomalous ones) provide relatively small and flat $\pi\Sigma$ mass distributions. It is the final state $MB$ rescattering (with the $K^{+}$ treated as a spectator) that is responsible for the peak structure and larger magnitude of the computed cross sections. A direct comparison of the generated $\pi\Sigma$ mass spectra with those reported by the CLAS collaboration [1] is currently finalized and will be presented at the meeting.

[1] K. Moriya et al. (CLAS Collaboration), Phys. Rev. C 88 (2013) 045201.
[2] N. Wickramaarachchi et al. (GlueX Collaboration), a talk at the HYP22 conference.
[3] P.C. Bruns, arXiv:2012.11298 [nucl-th].
[4] P.C. Bruns, A. Cieplý, Nucl. Phys. A 1019 (2022) 122378.
[5] S.X. Nakamura and D. Jido, PTEP 2014 (2014), 023D01; arXiv:1310.5768 [nucl-th].

Authors

Ales Cieply (Nuclear Physics Institute, Rez, Czechia) Peter C. Bruns (Nuclear Physics Institute, Rez, Czechia)

Presentation materials