Based on the observation that K_0(1412) is lighter than its SU_3 counterpart, a_0(1474), we examine the possibility that these particles, together with f_0(1370), f_0(1507) and f_0(1714), fill a tetraquark recurrence of the light 0^{++} nonet mixed with a glueball state. We find the picture to be better consistent than the qqbar hypothesis with the known data about the three f_0 resonances. Conventional spin-orbit coupling suggests the qqbar, P-wave, nonet to lie around 1200 MeV
The recent observations of f_0(980) in charmless B-decays motivate further studies of scalar particl...
The next to lowest mass scalar multiplet is treated as the $q\bar{q}$,$P$-wave nonet, weakly mixed w...
Abstract. Lattice QCD predictions have motivated several recent studies of the mixing between the pr...
In our phenomenological analysis of the spectroscopy of light scalar mesons we do not find compellin...
Lattice gauge calculations predict the existence of glueballs. In particular a scalar glueball is fi...
We discuss the classification of the light scalar mesons with mass below 2 GeV into q qbar nonets an...
We present a numerical solution of the four-quark Bethe–Salpeter equation for ground-state scalar te...
Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in...
Following the re-establishment of the \sigma(600) and the \kappa(900), the light scalar mesons a_0(9...
The possibility that gluonic excitations of hadronic matter or of the QCD vacuum may exist is perhap...
According to the QCD expectations the lightest glueball should be a scalar particle (J^{PC}=0^{++})....
AbstractWe present a numerical solution of the four-quark Bethe–Salpeter equation for ground-state s...
We study the possible tetraquark interpretation of light scalar meson states a(0)(980), f(0)(980), k...
We show that two nonets and a glueball provide a consistent description of data on scalar mesons bel...
Basing on the latest results of the PNPI (Gatchina) and QM&W College (London) groups, I discuss syst...
The recent observations of f_0(980) in charmless B-decays motivate further studies of scalar particl...
The next to lowest mass scalar multiplet is treated as the $q\bar{q}$,$P$-wave nonet, weakly mixed w...
Abstract. Lattice QCD predictions have motivated several recent studies of the mixing between the pr...
In our phenomenological analysis of the spectroscopy of light scalar mesons we do not find compellin...
Lattice gauge calculations predict the existence of glueballs. In particular a scalar glueball is fi...
We discuss the classification of the light scalar mesons with mass below 2 GeV into q qbar nonets an...
We present a numerical solution of the four-quark Bethe–Salpeter equation for ground-state scalar te...
Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in...
Following the re-establishment of the \sigma(600) and the \kappa(900), the light scalar mesons a_0(9...
The possibility that gluonic excitations of hadronic matter or of the QCD vacuum may exist is perhap...
According to the QCD expectations the lightest glueball should be a scalar particle (J^{PC}=0^{++})....
AbstractWe present a numerical solution of the four-quark Bethe–Salpeter equation for ground-state s...
We study the possible tetraquark interpretation of light scalar meson states a(0)(980), f(0)(980), k...
We show that two nonets and a glueball provide a consistent description of data on scalar mesons bel...
Basing on the latest results of the PNPI (Gatchina) and QM&W College (London) groups, I discuss syst...
The recent observations of f_0(980) in charmless B-decays motivate further studies of scalar particl...
The next to lowest mass scalar multiplet is treated as the $q\bar{q}$,$P$-wave nonet, weakly mixed w...
Abstract. Lattice QCD predictions have motivated several recent studies of the mixing between the pr...