Constraining the mass and width of the N∗(1685)N^*(1685) resonance

preprint2013arXivOpen access

Abstract

We have examined the existence of the N∗(1685)N^*(1685) resonance, which is recently listed by the Particle Data Group as a one-star nucleon resonance, by using a covariant isobar model for kaon photoproduction and assuming that the resonance has Jp=1/2+J^p=1/2^+, in accordance with our previous finding. After the inclusion of this resonance the changes in the total χ2χ^2 show two clear minima at MN∗=1650M_{N^*}=1650 and 1696 MeV, which correspond to two different resonance states. The former corresponds to the narrow nucleon resonance found in our previous investigation, whereas the latter corresponds to a new resonance found as we increase the resonance width. From the latter we derive the mass and width relation of the N∗(1685)N^*(1685) resonance. We observe that the properties of both the N∗(1685)N^*(1685) and N∗(1710)P11N^*(1710)P_{11} resonances are strongly correlated. Although the best fit of the present work yields MN∗=1696M_{N^*}=1696 MeV and ΓN∗=76Γ_{N^*}=76 MeV, the apparently small N∗(1710)P11N^*(1710)P_{11} coupling constant to the K+ΛK^+Λ channel found in previous investigations suggests that ΓN∗≲35Γ_{N^*}\lesssim 35 MeV, which, according to the mass and width relation, corresponds to MN∗≲1680M_{N^*}\lesssim 1680 MeV.

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