We study gauge boson propagators in the symmetric and symmetry broken phases of the 3-d, SU(2) gauge-Higgs model. Correlation functions for the gauge fields are calculated in Landau gauge. They are found to decay exponentially at large distances leading to a non-vanishing mass for the gauge bosons. We find that the W-boson screening mass drops in the symmetry broken phase when approaching the critical temperature. In the symmetric phase the screening mass stays small and is independent of the scalar--gauge coupling (the hopping parameter). Numerical results coincide with corresponding calculations performed for the pure gauge theory. We find m_w = 0.35(1)g^2T in this phase which is consistent with analytic calculations based on gap equation...
The 3-dimensional gauge-Higgs system describes the non-perturbative infrared effects of the high-tem...
Heller UM, Karsch F, Rank J. Gluon propagator at high temperature: Screening, improvement and nonzer...
The screening masses of hot SU(N) gauge theory, defined as poles of the corresponding propagators ar...
Karsch F, Neuhaus T, Patkos A, Rank J. Gauge boson masses in the 3D, SU(2) gauge-Higgs model. NUCLEA...
Karsch F, Neuhaus T, Patkos A, Rank J. Critical Higgs mass and temperature dependence of gauge boson...
We derive a set of gauge independent gap equations for Higgs boson and vector boson masses for the S...
Karsch F, Oevers M, Petreczky P. Screening masses of hot SU(2) gauge theory from the 3d adjoint Higg...
We calculate the masses of the low-lying states with quantum numbers JPC = 0++,1-- in the Higgs and ...
We calculate the masses of the low-lying states with quantum numbers JPC = 0++,1-- in the Higgs and ...
We calculate the masses of the low-lying states with quantum numbers J"P"C=0"+"+...
We study the spectrum of screening masses in the deconfined phase of (3+1)D SU(2) pure gauge theory ...
We study the electroweak phase transition by lattice simulations of an effective 3-dimensional theor...
We study the gluon propagator in Landau gauge in the deconfined phase of SU(2) gauge theory. From th...
The 3-dimensional gauge-Higgs system describes the non-perturbative infrared effects of the high-tem...
Numerical simulations are performed to study the finite temperature phase transition in the SU(2) Hi...
The 3-dimensional gauge-Higgs system describes the non-perturbative infrared effects of the high-tem...
Heller UM, Karsch F, Rank J. Gluon propagator at high temperature: Screening, improvement and nonzer...
The screening masses of hot SU(N) gauge theory, defined as poles of the corresponding propagators ar...
Karsch F, Neuhaus T, Patkos A, Rank J. Gauge boson masses in the 3D, SU(2) gauge-Higgs model. NUCLEA...
Karsch F, Neuhaus T, Patkos A, Rank J. Critical Higgs mass and temperature dependence of gauge boson...
We derive a set of gauge independent gap equations for Higgs boson and vector boson masses for the S...
Karsch F, Oevers M, Petreczky P. Screening masses of hot SU(2) gauge theory from the 3d adjoint Higg...
We calculate the masses of the low-lying states with quantum numbers JPC = 0++,1-- in the Higgs and ...
We calculate the masses of the low-lying states with quantum numbers JPC = 0++,1-- in the Higgs and ...
We calculate the masses of the low-lying states with quantum numbers J"P"C=0"+"+...
We study the spectrum of screening masses in the deconfined phase of (3+1)D SU(2) pure gauge theory ...
We study the electroweak phase transition by lattice simulations of an effective 3-dimensional theor...
We study the gluon propagator in Landau gauge in the deconfined phase of SU(2) gauge theory. From th...
The 3-dimensional gauge-Higgs system describes the non-perturbative infrared effects of the high-tem...
Numerical simulations are performed to study the finite temperature phase transition in the SU(2) Hi...
The 3-dimensional gauge-Higgs system describes the non-perturbative infrared effects of the high-tem...
Heller UM, Karsch F, Rank J. Gluon propagator at high temperature: Screening, improvement and nonzer...
The screening masses of hot SU(N) gauge theory, defined as poles of the corresponding propagators ar...