Why there is no spin-orbit inversion in heavy-light mesons?

Abstract

We show that the absence of spin-orbit inversions in heavy-light mesons can be explained by the chiral radiative corrections in potential model. A new potential model estimate is given of the masses for P-wave bottom mesons.

10 pages, published in PRD

Cited by in corpus (8)

• Spin-dependent interactions in quarkonia
• Structure of the $(0^{+},1^{+})$ mesons $B_{s0}$ and $B_{s1}$, and the strong coupling constants $g_{B_{s0}BK}$ and $g_{B_{s1}{B}^{\ast }K}$
• Energies of B_s meson excited states - a lattice study
• Reanalysis of the (0^+,1^+) states B_{s0} and B_{s1} with QCD sum rules
• Strong decays $B_{s0}\to B_s\pi$ and $B_{s1}\to B_s^{\ast }\pi$ with light-cone QCD sum rules
• Dynamical suppression of the spin-orbit interaction in hadrons
• Radiative decays of the $(0^{+},1^{+})$ strange-bottom mesons
• Chiral radiative corrections in potential model and the P-wave states of heavy-light mesons