# Some Phenomenological Aspects of Kaon Photoproduction in the Extreme   Kinematics

**Authors:** S. Sakinah, S. Clymton, T. Mart

arXiv: 1905.03675 · 2019-10-23

## TL;DR

This paper explores the phenomenological aspects of kaon photoproduction in extreme kinematic regions, analyzing amplitude convergence, and extracting coupling constants in forward and backward scattering regions.

## Contribution

It provides a detailed analysis of amplitude convergence in the threshold region and methods to extract coupling constants in forward and backward kinematics.

## Key findings

- Amplitude convergence requires expansion up to 12th order at threshold.
- Expansion impacts the extraction of coupling constants in different kinematic regions.
- Soft Kaon Approximation is not easily applicable in kaon photoproduction.

## Abstract

We have investigated phenomenological aspects of kaon photoproduction in three different extreme kinematics. The first kinematics of interest is the threshold region. At the threshold we have investigated the convergence of kaon photoproduction amplitude by expanding the square of the amplitude in terms of the ratio $m_K/m$, where $m_K$ is the mass of kaon and $m$ is the averaged mass of nucleon and $\Lambda$-hyperon. The amplitude is calculated from the appropriate Feynman diagrams by using the pseudovector theory. The contact diagram as a consequence of the PCAC hypothesis is also taken into account in the amplitude. Our finding indicates that the convergence can be only achieved if the amplitude was expanded up to at least $12^{\rm th}$ order. As a consequence, applications of some theoretical calculations based on the expansion the scattering amplitude, such as the Low Energy Theorem or Soft Kaon Approximation, cannot be easily managed in kaon photoproduction. The second kinematics is the forward region, where we could assume only $t$-channel contributes to the process. Here we have investigated the effect of amplitude expansion on the extraction of the coupling constants $g_{K^+\Lambda p}$ and $g^V_{K_1^+\Lambda p}$. The last kinematics is the backward region, where we have also assumed that only $u$-channel survives and we could extract the leading coupling constants $g_{K^+\Lambda p} $ and $g_{K^+\Sigma^0 p}$.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1905.03675/full.md

## References

33 references — full list in the complete paper: https://tomesphere.com/paper/1905.03675/full.md

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Source: https://tomesphere.com/paper/1905.03675