A survey of heavy–heavy hadronic molecules
Xiang-Kun Dong,Feng-Kun Guo,Bing-Song Zou
Table 8. The group theory factor F, defined in equation (13), for the interaction of charm–anticharm/charm–charm hadron pairs with only the light vector-meson exchanges. Here one of the charm hadrons is an sℓ = 3/2 charm meson. See the caption of table 7.
SystemISThresholds [MeV]Exchanged particlesF
${D}^{(* )}{\bar{D}}_{\mathrm{1,2}}$/D(*)D1,200/0(4289, 4330, 4431, 4472)ρ, ω$\tfrac{3}{2},\tfrac{1}{2}$/$\tfrac{3}{2},-\tfrac{1}{2}$
10/0$-\tfrac{1}{2},\tfrac{1}{2}$/ $-\tfrac{1}{2},-\tfrac{1}{2}$
${D}^{(* )}{\bar{D}}_{s1,s2}$/D(*)Ds1,s2$\tfrac{1}{2}$1/ − 1(4390, 4431, 4534, 4575)−0/0
${D}_{s}^{(* )}{\bar{D}}_{\mathrm{1,2}}$/${D}_{s}^{(* )}{D}_{\mathrm{1,2}}$$\tfrac{1}{2}$ − 1/1(4402, 4436, 4544, 4578)−0/0
${D}_{s}^{(* )}{\bar{D}}_{s1,s2}$/${D}_{s}^{(* )}{D}_{s1,s2}$00/−2(4503, 4537, 4647, 4681)φ1/−1
${D}_{\mathrm{1,2}}{\bar{D}}_{\mathrm{1,2}}$/D1,2D1,200/0(4844, 4885, 4926)ρ, ω$\tfrac{3}{2},\tfrac{1}{2}$/$\tfrac{3}{2},-\tfrac{1}{2}$
1$-\tfrac{1}{2},\tfrac{1}{2}$/$-\tfrac{1}{2},-\tfrac{1}{2}$
${D}_{s1,s2}{\bar{D}}_{\mathrm{1,2}}$/Ds1,s2D1,2$\tfrac{1}{2}$1/1(4957, 4991, 4998, 5032)0/0
${D}_{s1,s2}{\bar{D}}_{s1,s2}$/Ds1,s2Ds1,s200/ − 2(5070, 5104, 5138)φ1/1
${{\rm{\Lambda }}}_{c}{\bar{D}}_{\mathrm{1,2}}$/ΛcD1,2$\tfrac{1}{2}$0/0(4708, 4750)ω−1/1
${{\rm{\Lambda }}}_{c}{\bar{D}}_{s1,s2}$/ΛcDs1,s20 − 1/1(4822, 4856)−0/0
${{\rm{\Xi }}}_{c}{\bar{D}}_{\mathrm{1,2}}$/ξcD1,21 − 1/ − 1(4891, 4932)ρ, ω$-\tfrac{1}{2},-\tfrac{1}{2}$/$-\tfrac{1}{2},\tfrac{1}{2}$
0$\tfrac{3}{2},-\tfrac{1}{2}$/$\tfrac{3}{2},\tfrac{1}{2}$
${{\rm{\Xi }}}_{c}{\bar{D}}_{s1,s2}$/ξcDs1,s2$\tfrac{1}{2}$ − 2/0(5005, 5039)φ−1/1
${{\rm{\Sigma }}}_{c}^{(* )}{\bar{D}}_{\mathrm{1,2}}$/${{\rm{\Sigma }}}_{c}^{(* )}{D}_{\mathrm{1,2}}$$\tfrac{3}{2}$0/0(4876, 4917, 4940, 4981)ρ, ω − 1, − 1/ − 1, 1
$\tfrac{1}{2}$2, − 1/2,1
${{\rm{\Sigma }}}_{c}^{(* )}{\bar{D}}_{s1,s2}$/${{\rm{\Sigma }}}_{c}^{(* )}{D}_{s1,s2}$11/ − 1(4989, 5023, 5053, 5087)−0/0
${{\rm{\Xi }}}_{c}^{{\prime} (* )}{\bar{D}}_{\mathrm{1,2}}$/${{\rm{\Xi }}}_{c}^{{\prime} (* )}{D}_{\mathrm{1,2}}$1 − 1/ − 1(5001, 5042, 5068, 5109)ρ, ω$-\tfrac{1}{2},-\tfrac{1}{2}$/$-\tfrac{1}{2},\tfrac{1}{2}$
0$\tfrac{3}{2},-\tfrac{1}{2}$/$\tfrac{3}{2},\tfrac{1}{2}$
${{\rm{\Xi }}}_{c}^{{\prime} (* )}{\bar{D}}_{s1,s2}$/${{\rm{\Xi }}}_{c}^{{\prime} (* )}{D}_{s1,s2}$$\tfrac{1}{2}$ − 2/0(5114, 5148, 5181, 5215)φ−1/1
${{\rm{\Omega }}}_{c}^{(* )}{\bar{D}}_{\mathrm{1,2}}$/${{\rm{\Omega }}}_{c}^{(* )}{D}_{\mathrm{1,2}}$$\tfrac{1}{2}$ − 2/ − 2(5117, 5158, 5188, 5229)−0/0
${{\rm{\Omega }}}_{c}^{(* )}{\bar{D}}_{s1,s2}$/${{\rm{\Omega }}}_{c}^{(* )}{D}_{s1,s2}$0 − 3/ − 1(5230, 5264, 5301, 5335)φ−2/2