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- W2008524067 endingPage "2695" @default.
- W2008524067 startingPage "2687" @default.
- W2008524067 abstract "Suzuka and Sugawara's theory of $S$-wave nonleptonic hyperon decay is reviewed to see to what extent their theory tests current algebra and the currentifmmodetimeselsetexttimesfi{}current form of interaction. The only argument for the currentifmmodetimeselsetexttimesfi{}current form in nonleptonic decays that it is all compelling is the vanishing of the $S$-wave amplitude $A({{ensuremath{Sigma}}_{+}}^{+})$ for the decay ${ensuremath{Sigma}}^{+}ensuremath{rightarrow}n+{ensuremath{pi}}^{+}$. For the $P$-wave decay, to which the soft-pion formalism is inapplicable, an octet pole model is used. To fit the empirical $P$-wave amplitudes, strong-coupling shifts are required in both the $S$ and the $P$ waves. Including $mathrm{SU}(3)$ symmetry breaking leads to parity-violating Born terms in the $S$ waves; to estimate the parity-violating spurion coupling, the kaon tadpole model and ${K}_{2}ensuremath{pi}$ decay rate are used. If pionic and kaonic strong-coupling constants are suppressed by $frac{2}{3}$ and $frac{1}{3}$, all the $S$- and $P$-wave amplitudes are given within 20%, but $A({{ensuremath{Sigma}}_{+}}^{+})$ now does not precisely vanish. If $A({{ensuremath{Sigma}}_{+}}^{+})=0$ exactly is insisted on, then the suppression of pionic strong-coupling constants by $frac{2}{3}$ and $frac{1}{3}$ is necessary." @default.
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- W2008524067 date "1970-05-01" @default.
- W2008524067 modified "2023-09-25" @default.
- W2008524067 title "Nonleptonic Hyperon Decays" @default.
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- W2008524067 doi "https://doi.org/10.1103/physrevd.1.2687" @default.
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