Pseudovector versus pseudoscalar theory in kaon photoproduction from nucleons and nuclei
C. Bennhold, L. E. Wright
Abstract
C. Bennhold, L. E. Wright
Abstract
The reaction $^{1}\mathrm{H}$(\ensuremath{\gamma},${\mathrm{K}}^{+}$)${\mathrm{\ensuremath{\Lambda}}}^{0}$ is used to compare pseudovector with pseudoscalar coupling for the K\ensuremath{\Lambda}N vertex. The operator is based on diagrammatic techniques and includes the Born terms along with the ${\mathrm{K}}^{\mathrm{*}}$ and \ensuremath{\Sigma} exchange terms. Obtaining the coupling constants from a least squares fit shows that the data do not prefer one coupling over the other. Implanting the process into the nucleus yields only small differences between the two interactions.
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The reaction $^{1}\mathrm{H}$(\ensuremath{\gamma},${\mathrm{K}}^{+}$)${\mathrm{\ensuremath{\Lambda}}}^{0}$ is used to compare pseudovector with pseudoscalar coupling for the K\ensuremath{\Lambda}N vertex. The operator is based on diagrammatic techniques and includes the Born terms along with the ${\mathrm{K}}^{\mathrm{*}}$ and \ensuremath{\Sigma} exchange terms. Obtaining the coupling constants from a least squares fit shows that the data do not prefer one coupling over the other. Implanting the process into the nucleus yields only small differences between the two interactions.
Key concepts: Pseudovector, Pseudoscalar, Physics, Nucleon, Lambda, Particle physics, Coupling constant, Vertex (graph theory)