K*Σ* molecular states form in the I=3/2 channel for several J^P values and may explain the N(2250) and Δ(2200) resonances.
As shown in Table IV, for the isospin I = 1/ 2 and JP = 1/ 2−channel, which corresponds to the S -wave K∗Σ∗molec- ular configuration, no stable bound-state solution is found
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The possible $K^{*}\Sigma^{*}$ molecular state
K*Σ* molecular states form in the I=3/2 channel for several J^P values and may explain the N(2250) and Δ(2200) resonances.