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Coupled-channel analysis of the possible D(∗)D(∗)D^{(*)}D^{(*)}, Bˉ(∗)Bˉ(∗)\bar{B}^{(*)}\bar{B}^{(*)} and D(∗)Bˉ(∗)D^{(*)}\bar{B}^{(*)} molecular states

Abstract

We perform a coupled-channel study of the possible deuteron-like molecules with two heavy flavor quarks, including the systems of D(∗)D(∗)D^{(*)}D^{(*)} with double charm, Bˉ(∗)Bˉ(∗)\bar{B}^{(*)}\bar{B}^{(*)} with double bottom and D(∗)Bˉ(∗)D^{(*)}\bar{B}^{(*)} with both charm and bottom, within the one-boson-exchange model. In our study, we take into account the S-D mixing which plays an important role in the formation of the loosely bound deuteron, and particularly, the coupled-channel effect in the flavor space. According to our calculation, the states D(∗)D(∗)[I(JP)=0(1+)]D^{(*)}D^{(*)}[I(J^P)=0(1^+)] and (D(∗)D(∗))s[JP=1+](D^{(*)}D^{(*)})_s[J^P=1^+] with double charm, the states Bˉ(∗)Bˉ(∗)[I(JP)=0(1+),0(2+),1(0+),1(1+),1(2+)]\bar{B}^{(*)}\bar{B}^{(*)}[I(J^P)=0(1^+),0(2^+),1(0^+),1(1^+),1(2^+)], (Bˉ(∗)Bˉ(∗))s[JP=0+,1+,2+](\bar{B}^{(*)}\bar{B}^{(*)})_s[J^P=0^+,1^+,2^+] and (Bˉ(∗)Bˉ(∗))ss[JP=0+,1+,2+](\bar{B}^{(*)}\bar{B}^{(*)})_{ss}[J^P=0^+,1^+,2^+] with double bottom, and the states D(∗)Bˉ(∗)[I(JP)=0(0+),0(1+)]D^{(*)}\bar{B}^{(*)}[I(J^P)=0(0^+),0(1^+)] and (D(∗)Bˉ(∗))s[JP=0+,1+](D^{(*)}\bar{B}^{(*)})_s[J^P=0^+,1^+] with both charm and bottom are good molecule candidates. However, the existence of the states D(∗)D(∗)[I(JP)=0(2+)]D^{(*)}D^{(*)}[I(J^P)=0(2^+)] with double charm and D(∗)Bˉ(∗)[I(JP)=1(1+)]D^{(*)}\bar{B}^{(*)}[I(J^P)=1(1^+)] with both charm and bottom is ruled out.Comment: 1 figure added, published in Physical Review

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