Chiral symmetry and its spontaneous breaking play an important role both in the light
hadron and heavy hadron systems. The chiral perturbation theory (χ PT) is the low energy …

Since the discovery of the first charmed meson in 1976, many open-charm and open-bottom
hadrons were observed. In 2003 two narrow charm-strange states $ D_ {s0}^{\ast}(2317) …

Motivated by the success of the flavour physics programme carried out over the last decade
at the Large Hadron Collider (LHC), we characterize in detail the physics potential of its High …

Single-and double-heavy baryons are studied in the constituent quark model. The model
Hamiltonian is chosen as a standard one with two exceptions:(1) the color-Coulomb term …

The large number of B c mesons observed by LHCb suggests a sizable cross section for
producing doubly heavy baryons in the same experiment. Motivated by this, we estimate …

We calculate the masses of the(;) tetraquark states with the aid of heavy diquark-antiquark
symmetry (HDAS) and the chromomagnetic interaction (CMI) model. The masses of the …

A quark model is applied to the spectrum of baryons containing heavy quarks. The model
gives masses for the known heavy baryons that are in agreement with experiment, but for …

We calculate the masses of baryons containing one, two, or three heavy quarks using lattice
QCD. We consider all possible combinations of charm and bottom quarks, and compute a …

We discuss the mass spectrum of Ω Ω baryon with two heavy quarks and one light quark
(ccs, bbs, and bcs). The main goal of the paper is to calculate the ground state masses and …

In this paper we compute masses and magnetic moments of heavy baryons and tetraquarks
with one and two open heavy flavors in a unified framework of the MIT bag model. Using the …