A survey of heavy–heavy hadronic molecules
Xiang-Kun Dong,Feng-Kun Guo,Bing-Song Zou
Table 10. The group theory factor F, defined in equation (13), for the interaction of bottom–antibottom/bottom–bottom hadron pairs with only the light vector-meson exchanges. Here one of the bottom hadrons is an sℓ = 3/2 bottom meson. See the caption of table 9.
SystemISThresholds [MeV]Exchanged particlesF
${B}^{(* )}{\bar{B}}_{\mathrm{1,2}}$/B(*)B1,200/0(11005, 11051, 11018, 11063)ρ, ω$\tfrac{3}{2},\tfrac{1}{2}$/$\tfrac{3}{2},-\tfrac{1}{2}$
10/0$-\tfrac{1}{2},\tfrac{1}{2}$/ $-\tfrac{1}{2},-\tfrac{1}{2}$
${B}^{(* )}{\bar{B}}_{s1,s2}$/B(*)Bs1,s2$\tfrac{1}{2}$1/ − 1(11093, 11141, 11105, 11154)−0/0
${B}_{s}^{(* )}{\bar{B}}_{\mathrm{1,2}}$/${B}_{s}^{(* )}{B}_{\mathrm{1,2}}$$\tfrac{1}{2}$ − 1/1(11108, 11153, 11119, 11165)−0/0
${B}_{s}^{(* )}{\bar{B}}_{s1,s2}$/${B}_{s}^{(* )}{B}_{s1,s2}$00/−2(11196, 11207, 11244, 11255)φ1/−1
${B}_{\mathrm{1,2}}{\bar{B}}_{\mathrm{1,2}}$/B1,2B1,200/0(11452, 11464, 11477)ρ, ω$\tfrac{3}{2},\tfrac{1}{2}$/$\tfrac{3}{2},-\tfrac{1}{2}$
1$-\tfrac{1}{2},\tfrac{1}{2}$/$-\tfrac{1}{2},-\tfrac{1}{2}$
${B}_{s1,s2}{\bar{B}}_{\mathrm{1,2}}$/Bs1,s2B1,2$\tfrac{1}{2}$1/1(11555, 11566, 11567, 11578)0/0
${B}_{s1,s2}{\bar{B}}_{s1,s2}$/Bs1,s2Bs1,s200/ − 2(11657, 11669, 11680)φ1/1
${{\rm{\Lambda }}}_{b}{\bar{B}}_{\mathrm{1,2}}$/ΛbB1,2$\tfrac{1}{2}$0/0(11346, 11358)ω−1/1
${{\rm{\Lambda }}}_{b}{\bar{B}}_{s1,s2}$/ΛbBs1,s20 − 1/1(11448, 11459)−0/0
${{\rm{\Xi }}}_{b}{\bar{B}}_{\mathrm{1,2}}$/ξbB1,21 − 1/ − 1(11520, 11533)ρ, ω$-\tfrac{1}{2},-\tfrac{1}{2}$/$-\tfrac{1}{2},\tfrac{1}{2}$
0$\tfrac{3}{2},-\tfrac{1}{2}$/$\tfrac{3}{2},\tfrac{1}{2}$
${{\rm{\Xi }}}_{b}{\bar{B}}_{s1,s2}$/ξbBs1,s2$\tfrac{1}{2}$ − 2/0(11623, 11634)φ−1/1
${{\rm{\Sigma }}}_{b}^{(* )}{\bar{B}}_{\mathrm{1,2}}$/${{\rm{\Sigma }}}_{b}^{(* )}{B}_{\mathrm{1,2}}$$\tfrac{3}{2}$0/0(11539, 11551, 11559, 11571)ρ, ω − 1, − 1/ − 1, 1
$\tfrac{1}{2}$2, − 1/2,1
${{\rm{\Sigma }}}_{b}^{(* )}{\bar{B}}_{s1,s2}$/${{\rm{\Sigma }}}_{b}^{(* )}{B}_{s1,s2}$11/ − 1(11642, 11653, 11661, 11672)−0/0
${{\rm{\Xi }}}_{b}^{{\prime} (* )}{\bar{B}}_{\mathrm{1,2}}$/${{\rm{\Xi }}}_{b}^{{\prime} (* )}{B}_{\mathrm{1,2}}$1 − 1/ − 1(11661, 11673, 11680, 11692)ρ, ω$-\tfrac{1}{2},-\tfrac{1}{2}$/$-\tfrac{1}{2},\tfrac{1}{2}$
0$\tfrac{3}{2},-\tfrac{1}{2}$/$\tfrac{3}{2},\tfrac{1}{2}$
${{\rm{\Xi }}}_{b}^{{\prime} (* )}{\bar{B}}_{s1,s2}$/${{\rm{\Xi }}}_{b}^{{\prime} (* )}{B}_{s1,s2}$$\tfrac{1}{2}$ − 2/0(11764, 11775, 11783, 11794)φ−1/1
${{\rm{\Omega }}}_{b}^{(* )}{\bar{B}}_{\mathrm{1,2}}$/${{\rm{\Omega }}}_{b}^{(* )}{B}_{\mathrm{1,2}}$$\tfrac{1}{2}$ − 2/ − 2(11772, 11784, 11796, 11808)−0/0
${{\rm{\Omega }}}_{b}^{(* )}{\bar{B}}_{s1,s2}$/${{\rm{\Omega }}}_{b}^{(* )}{B}_{s1,s2}$0 − 3/ − 1(11875, 11886, 11899, 11910)φ−2/2