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Molecular pentaquark states with open charm and bottom flavors

Published 2 Aug 2023 in hep-ph and hep-ex | (2308.01007v3)

Abstract: We study the possibly-existing molecular pentaquark states with open charm and bottom flavors, {\it i.e.}, the states with the quark contents cbˉqqqc\bar{b}qqq and bcˉqqqb\bar{c}qqq (q=u,d,sq=u,d,s). We investigate the meson-baryon interactions through the coupled-channel unitary approach within the local hidden-gauge formalism, and extract the poles by solving the Bethe-Salpeter equation in coupled channels. These poles qualify as molecular pentaquark states, which are dynamically generated from the meson-baryon interactions through the exchange of vector mesons. Our results suggest the existence of the Σc<sup>(∗)</sup>B<sup>(∗)\Sigma_c<sup>{(*)}</sup> B<sup>{(*)} and Σb<sup>(∗)</sup>Dˉ<sup>(∗)\Sigma_b<sup>{(*)}</sup> \bar{D}<sup>{(*)} molecular states with isospin I=1/2I=1/2, the Ξc<sup>(′,∗)</sup>B<sup>(∗)\Xi_c<sup>{(\prime,*)}</sup> B<sup>{(*)} and Ξb<sup>(′,∗)</sup>Dˉ<sup>(∗)\Xi_b<sup>{(\prime,*)}</sup> \bar{D}<sup>{(*)} molecular states with isospin I=0I=0 and I=1I=1, as well as the Ωc<sup>(∗)</sup>B<sup>(∗)\Omega_c<sup>{(*)}</sup> B<sup>{(*)} and Ωb<sup>(∗)</sup>Dˉ<sup>(∗)\Omega_b<sup>{(*)}</sup> \bar D<sup>{(*)} molecular states with isospin I=1/2I=1/2.

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