Analysis of J/ψ → Λ π Σ-bar finds Σ(1385) and Σ(1430) signals but shows the Σ(1380) is unnecessary when π Σ-bar interactions are accounted for.
Moriyaet al.[CLAS], Phys
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Phenomenological model of charmed baryon decay reproduces data and predicts cusp signature of dynamically generated Σ*(1/2⁻) resonance.
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Identifying $\Sigma(1380)$ and $\Sigma(1430)$ in the $J/\psi \to \Lambda \pi \bar{\Sigma}$ reaction
Analysis of J/ψ → Λ π Σ-bar finds Σ(1385) and Σ(1430) signals but shows the Σ(1380) is unnecessary when π Σ-bar interactions are accounted for.
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Search for the low-lying excited baryon $\Sigma^*(1/2^-)$ through process $\Lambda^+_c \to \Lambda K^0 \pi^+$
Phenomenological model of charmed baryon decay reproduces data and predicts cusp signature of dynamically generated Σ*(1/2⁻) resonance.