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) …

The composite nature of baryons manifests itself in the existence of a rich spectrum of
excited states, in particular in the important mass region 1–2 GeV for the light-flavoured …

The recent experimental measurements on pp collisions at s= 5.02 TeV have shown a very
large production of heavy baryons corresponding to a Λ c/D 0 ratio of about 0.5. This ratio is …

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 …

Starting with the dynamical picture of the exotic cc¯-containing states XYZ as the
confinement-induced hadronization of a rapidly separating pair of a compact diquark and …

Several transport models have been employed in recent years to analyze heavy-flavor
meson spectra in high-energy heavy-ion collisions. Heavy-quark transport coefficients …

We have studied the meson-baryon S− wave interaction in the isoscalar hidden-charm
strange sector with the coupled-channels, η c Λ, J/ψ Λ, D¯ Ξ c, D¯ s Λ c, D¯ Ξ c′, D¯⁎ Ξ c …

In a coalescence plus fragmentation approach we calculate the heavy baryon/meson ratio
and the p_T p T spectra of charmed hadrons D^ 0 D 0, D_ s D s and\varLambda _ c^+ Λ c+ …

We investigate the structure of heavy baryons containing a charm or a bottom quark. We
employ a constituent quark model successful in the description of the baryon–baryon …

We present results for different observables measured in semileptonic and nonleptonic
decays of the B c-meson. The calculations have been done within the framework of a …