https://doi.org/10.1140/epjc/s10052-017-5252-4
Regular Article - Theoretical Physics
Masses of scalar and axial-vector B mesons revisited
1
Institute of Physics, Academia Sinica, Taipei, 115, Taiwan, Republic of China
2
School of Nuclear Science and Technology, Lanzhou University, Lanzhou, 730000, People’s Republic of China
* e-mail: yufsh@lzu.edu.cn
Received:
2
August
2017
Accepted:
22
September
2017
Published online:
7
October
2017
The SU(3) quark model encounters a great challenge in describing even-parity mesons. Specifically, the quark model has difficulties in understanding the light scalar mesons below 1 GeV, scalar and axial-vector charmed mesons and
charmonium-like state X(3872). A common wisdom for the resolution of these difficulties lies on the coupled channel effects which will distort the quark model calculations. In this work, we focus on the near mass degeneracy of scalar charmed mesons,
and
, and its implications. Within the framework of heavy meson chiral perturbation theory, we show that near degeneracy can be qualitatively understood as a consequence of self-energy effects due to strong coupled channels. Quantitatively, the closeness of
and
masses can be implemented by adjusting two relevant strong couplings and the renormalization scale appearing in the loop diagram. Then this in turn implies the mass similarity of
and
mesons. The
interaction with the Goldstone boson is crucial for understanding the phenomenon of near degeneracy. Based on heavy quark symmetry in conjunction with corrections from QCD and
effects, we obtain the masses of
and
mesons, for example,
,
with
being
corrections. We find that the predicted mass difference of 48 MeV between
and
is larger than that of 20–30 MeV inferred from the relativistic quark models, whereas the difference of 15 MeV between the central values of
and
is much smaller than the quark model expectation of 60–100 MeV. Experimentally, it is important to have a precise mass measurement of
mesons, especially the neutral one, to see if the non-strange scalar charmed meson is heavier than the strange partner as suggested by the recent LHCb measurement of the
.
© The Author(s), 2017