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The Peak Structure in the In-Flight ${}^{3}\text{He} ( K^{-} , \, Λp ) n$ Reaction Around the $\bar{K} N N$ Threshold

Published 21 Nov 2016 in nucl-th, hep-ph, and nucl-ex | (1611.07361v1)

Abstract: We theoretically investigate the origin of the peak structure around the $K{-} p p$ threshold observed in the in-flight ${}{3}\text{He} ( K{-} , \, \Lambda p ) n$ reaction in the recent E15 experiment at J-PARC. For this purpose, we consider two scenarios to produce the peak. One is that the $\Lambda (1405)$ is generated but it does not correlate with $p$, and the uncorrelated $\Lambda (1405) p$ system subsequently decays into $\Lambda p$. The other one is that the $\bar{K} N N$ bound state is indeed generated and decays into $\Lambda p$. As a result, the experimental signal is qualitatively well reproduced in the $\bar{K} N N$ bound scenario, definitely discarding the uncorrelated $\Lambda (1405) p$ one.

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