It is shown that the mass difference between η′ and pseudoscalar octet mesons can be calculated in quenched lattice QCD with the aid of a variant wall source technique. The estimated mass difference increases as the quark mass decreases, and its value extrapolated to the zero-quark-mass limit. mη′2-m82=(750±40 MeV)2, is close to the value determined from experiment (850 MeV)2. These results indicate that the long-standing U(1) problem could be solved in lattice QCD, with its essential part being understood within the quenched approximation. We also comment on implications of our results on spurious infrared divergences in quenched QCD
We present details of simulations for the light hadron spectrum in quenched QCD carried out on the C...
We compute decay constants of heavy–light mesons in quenched lattice QCD with a lattice spacing of a...
Using lattice QCD simulation in the quenched approximation, we study the κ meson, which is ^3P_0 in ...
It is shown that the mass difference between η′ and pseudoscalar octet mesons can be calculated in q...
If the sigma meson exists, it is natural to consider the κ meson as member of the nonet scalar state...
We compute the strange quark mass ms and the average of the u and d quark masses m̂ using full latti...
We investigate in lattice QCD the U(1) problem that the η’ meson (960 MeV) is much heavier than the ...
We present the details of simulations for the light hadron spectrum in quenched QCD carried out on t...
A fully non-perturbative lattice determination of the up/down and strange quark masses is given for ...
We compare flavour singlet and non-singlet vector mesons from first principles using lattice QCD. Wi...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
AbstractWe compute the strange and the average up/down quark masses in the quenched approximation of...
We perform a lattice mass analysis in the flavor singlet pseudoscalar channel on the SESAM and TχL f...
The low-energy spectrum and phenomenology of strongly-interacting particles is well described by Qu...
We present details of simulations for the light hadron spectrum in quenched QCD carried out on the C...
We compute decay constants of heavy–light mesons in quenched lattice QCD with a lattice spacing of a...
Using lattice QCD simulation in the quenched approximation, we study the κ meson, which is ^3P_0 in ...
It is shown that the mass difference between η′ and pseudoscalar octet mesons can be calculated in q...
If the sigma meson exists, it is natural to consider the κ meson as member of the nonet scalar state...
We compute the strange quark mass ms and the average of the u and d quark masses m̂ using full latti...
We investigate in lattice QCD the U(1) problem that the η’ meson (960 MeV) is much heavier than the ...
We present the details of simulations for the light hadron spectrum in quenched QCD carried out on t...
A fully non-perturbative lattice determination of the up/down and strange quark masses is given for ...
We compare flavour singlet and non-singlet vector mesons from first principles using lattice QCD. Wi...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
We calculate meson and baryon masses in quenched QCD for the small quark masses of phenomenological ...
AbstractWe compute the strange and the average up/down quark masses in the quenched approximation of...
We perform a lattice mass analysis in the flavor singlet pseudoscalar channel on the SESAM and TχL f...
The low-energy spectrum and phenomenology of strongly-interacting particles is well described by Qu...
We present details of simulations for the light hadron spectrum in quenched QCD carried out on the C...
We compute decay constants of heavy–light mesons in quenched lattice QCD with a lattice spacing of a...
Using lattice QCD simulation in the quenched approximation, we study the κ meson, which is ^3P_0 in ...