We study the potential of a static quark anti-quark pair in the confinement ''phase'' of the SU(2) Higgs model. Around separation r_b, the confining string of the gauge field breaks by formation of a dynamical pair of light quarks. The ground state and first excited state static potentials are determined by a variational technique from a matrix correlation in which suitably smeared gauge and Higgs fields enter. Our results at #beta# = 2.4 clearly show string breaking (r_b #approx# 1.9r_0). The investigation of properly defined overlaps confirms the interpretation of string breaking as a level crossing phenomenon between string-type and meson-type states. We study the scaling properties of the static potentials along a line of constant physi...
The static potential V(r) between a static quark and a static antiquark separated by a distance r is...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
We present results of our ongoing determination of string breaking in full QCD with Nf = 2 Wilson fe...
We study the fundamental potential in the confinement “phase” of the SU(2) Higgs model. Around separ...
We study the fundamental potential in the confinement “phase” of the SU(2) Higgs model. Around separ...
The static potential in the confinement ''phase'' of the SU(2) Higgs model is studied. In particular...
The static potential in the confinement ``phase of the SU(2) Higgs model is studied. In particular, ...
We present results for the ground state and first excited state static potentials in the confinement...
We present results for the ground state and first excited state static potentials in the confinement...
We present results for the static potential in the confinement phase of the SU(2) Higgs model on the...
We investigate the static potential in the confinement phase of the SU(2) Higgs model on the lattice...
We investigate the static potential in the confinement phase of the SU(2) Higgs model on the lattice...
In quantum chromodynamics (QCD), the static potential V (r) is de?ned as the energy of the ground st...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
The static potential V(r) between a static quark and a static antiquark separated by a distance r is...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
We present results of our ongoing determination of string breaking in full QCD with Nf = 2 Wilson fe...
We study the fundamental potential in the confinement “phase” of the SU(2) Higgs model. Around separ...
We study the fundamental potential in the confinement “phase” of the SU(2) Higgs model. Around separ...
The static potential in the confinement ''phase'' of the SU(2) Higgs model is studied. In particular...
The static potential in the confinement ``phase of the SU(2) Higgs model is studied. In particular, ...
We present results for the ground state and first excited state static potentials in the confinement...
We present results for the ground state and first excited state static potentials in the confinement...
We present results for the static potential in the confinement phase of the SU(2) Higgs model on the...
We investigate the static potential in the confinement phase of the SU(2) Higgs model on the lattice...
We investigate the static potential in the confinement phase of the SU(2) Higgs model on the lattice...
In quantum chromodynamics (QCD), the static potential V (r) is de?ned as the energy of the ground st...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
The static potential V(r) between a static quark and a static antiquark separated by a distance r is...
We numerically investigate the transition of the static quark-antiquark string into a static-light m...
We present results of our ongoing determination of string breaking in full QCD with Nf = 2 Wilson fe...