We present mass spectrum and magnetic moments of the n¯ n¯ QQ states, where n= u, d, s
and Q= c, b. We solve four-body Schrödinger equation with a quark potential model by using …

We calculate the 1 D, 2 P, and 2 S mass spectra of the singly bottom baryons and their
strong decay widths. The calculations are performed within a harmonic oscillator quark …

Masses of positive-parity and negative-parity diquarks are investigated at finite temperature
with a quark chemical potential. We employ the three-flavor Nambu-Jona-Lasinio model, in …

Effects of the U (1) A axial anomaly on the mass spectrum of singly heavy baryons (SHBs) is
studied in terms of the chiral effective theory based on the chiral linear representation for …

We investigate two-pion emission decays of singly charmed and bottom baryons, focusing
on Λ Q*(1 P) and Ξ Q*(1 P) states with JP= 1/2-and 3/2-, which belong to the flavor triplet 3¯ …

Masses of the singly heavy baryons (SHBs), composed of a heavy quark and a light diquark,
are studied from the viewpoints of heavy-quark spin symmetry (HQSS) and chiral-symmetry …

Chiral effective theory of light diquarks is revisited. We construct an effective Lagrangian
based on the linear representation of three-flavor chiral symmetry. Here, we focus on the …

We present a study of two-body decay widths of heavy baryons into another heavy baryon
and a light pseudoscalar meson in the framework of the non-relativistic quark model in …

We conduct an investigation on the spin $\frac {3}{2}\rightarrow\frac {1}{2} $ semileptonic
weak transition of single heavy baryons for the exclusive decay $\Sigma_ {b} …

Quarks are one of the elemental particles, and are the fundamental constituents of matter.
Quarks have six types which is called flavor, and they are classified as up (u) and down (d) …