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• W3100220957 abstract "Using separable $bar{K}N-piSigma$ potentials in the Faddeev equations, we calculated the binding energies and widths of the $K^{-}pp$, $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states on the basis of three- and four-body Alt-Grassberger-Sandhas equations in the momentum representation. One- and two-pole version of $bar{K}N-piSigma$ interaction are considered and the dependence of the resulting few-body energy on the two-body $bar{K}N-piSigma$ potential was investigated. The $s$-wave [3+1] and [2+2] sub-amplitudes are obtained by using the Hilbert-Schmidt expansion procedure for the integral kernels. As a result, we found a four-body resonance of the $K^{-}ppn$ and $K^{-}ppp$ quasi-bound states with a binding energy in the range $B_{K^{-}ppn}sim{55-70}$ and $B_{K^{-}ppp}sim{90-100}$ MeV, respectively. The calculations yielded full width of $Gamma_{K^{-}ppn}sim{16-20}$ and $Gamma_{K^{-}ppp}sim{7-20}$ MeV." @default.
• W3100220957 created "2020-11-23" @default.
• W3100220957 creator A5028167086 @default.
• W3100220957 creator A5063998697 @default.
• W3100220957 date "2016-09-01" @default.
• W3100220957 modified "2023-09-27" @default.
• W3100220957 title "Coupled-channels Faddeev AGS calculation of K-ppn and K-ppp quasi-bound states" @default.
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• W3100220957 doi "https://doi.org/10.1140/epja/i2016-16282-y" @default.
• W3100220957 hasPublicationYear "2016" @default.
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