Abstract
AbstractWe investigate the mass spectrum and the decay properties of the$$B_s$$Bsmesons within the screened nonrelativistic quark model and the$$^3P_0$$3P0model. Our results suggest that the$$B_{sJ}(6064)$$BsJ(6064)and$$B_{sJ}(6114)$$BsJ(6114)states, as the first solution of the recently LHCb measurements, could be explained as the$$B_s(1^3D_3)$$Bs(13D3)and$$B_s(1^3D_1)$$Bs(13D1), respectively. In addition, the$$B_{sJ}(6109)$$BsJ(6109)and$$B_{sJ}(6158)$$BsJ(6158)states, as the second solution of the LHCb measurements, could be explained as the$$B_{s2}^\prime (1D)$$Bs2′(1D)and$$B_{s1}(2P)$$Bs1(2P), respectively. Meanwhile, the$$B_{s1}(5830)$$Bs1(5830)could be interpreted as the candidate of the$$B_{s1}(1P)$$Bs1(1P). We also calculated the decay properties of the other excited$$B_s$$Bsmesons with the predicted masses, which should be helpful for the experimental searching in future.
Funder
Natural Science Foundation of Henan Province
Publisher
Springer Science and Business Media LLC
Subject
Physics and Astronomy (miscellaneous),Engineering (miscellaneous)