Why there is no spin-orbit inversion in heavy-light mesons?
arXiv:hep-ph/0612345 · doi:10.1103/PhysRevD.76.014017
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
References in corpus (6)
- Excited Heavy-Light Systems and Hadronic Transitions
- Study of B- => D**0 pi-(D**0 => D(*)+ pi-) decays
- Mass spectrum of orbitally and radially excited heavy-light mesons in the relativistic quark model
- Measurement of Masses and Widths of Excited Charm Mesons and Evidence for Broad States
- A relativistic chiral quark model for pseudoscalar emission from heavy mesons
- Chiral radiative corrections and D_s(2317)/D(2308) mass puzzle
Cited by in corpus (15)
- Spin-dependent interactions in quarkonia
- Masses of Scalar and Axial-Vector B Mesons Revisited
- Structure of the mesons and , and the strong coupling constants and
- Combined study of and open-charm mesons with natural spin-parity
- Near Mass Degeneracy in the Scalar Meson Sector: Implications for and Mesons
- Exclusive semileptonic decays on the lattice
- -hadron spectroscopy study based on the similarity of double bottom baryon and bottom meson
- Energies of B_s meson excited states - a lattice study
- The Strong Decays of Orbitally Excited Mesons by Improved Bethe-Salpeter Method
- Analysis of the heavy tensor meson's strong decay with QCD sum rules
- Reanalysis of the (0^+,1^+) states B_{s0} and B_{s1} with QCD sum rules
- Strong decays and with light-cone QCD sum rules
- Radiative decays of the strange-bottom mesons
- Dynamical suppression of the spin-orbit interaction in hadrons
- Chiral radiative corrections in potential model and the P-wave states of heavy-light mesons