The recent observation at CDF and D0 of Σ b, Σ b* and Ξ b baryons opens the door to the
advent of new states in the bottom baryon sector. The states measured provide sufficient …

The first hyperon was discovered about 70 years ago, but the nature of these particles,
particularly with regard to multistrange hyperons, and many of their properties can still be …

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 a quark model calculation of the charmonium spectrum with self-energy
corrections due to the coupling to the meson-meson continuum. The bare masses used in …

We present a generalization of the hyperspherical harmonic formalism to study systems
made of quarks and antiquarks of the same flavor. This generalization is based on the …

We present an exact calculation of S and P wave QQ n¯ n¯ states using different standard
nonrelativistic quark-quark potentials. We explore in detail the charm and bottom sectors …

We show the results of a coupled-channel quark model calculation of the bottomonium
spectrum with self-energy corrections due to the coupling to the meson-meson continuum …

Strange and nonstrange baryon spectra in the relativistic interacting quark-diquark model with a
Gürsey and Radicati-inspired e Page 1 PHYSICAL REVIEW C 92, 025202 (2015) Strange and …

We present recent results of hadron spectroscopy and hadron–hadron interaction from the
perspective of constituent quark models. We pay special attention to the role played by …

Abstract The Z_ c (3900)^ ±/Z_c (3885)^ ± Z c (3900)±/Z c (3885)±and Z_ c (4020)^ ± Z c
(4020)±are two charmonium-like structures discovered in the π J/ψ π J/ψ and D^* ̄ D^(*)+ …