Karsch F, Oevers M, Petreczky P. Screening masses of hot SU(2) gauge theory from the 3d adjoint Higgs model. PHYSICS LETTERS B. 1998;442(1-4):291-299.We study the Landau gauge propagators of the lattice SU(2) 3d adjoint Higgs model, considered as an effective theory of high temperature 4d SU(2) gauge theory. From the long distance behaviour of the propagators we extract the screening masses. The propagators are studied both in the symmetric and the broken phases of the 3d Higgs model. It is shown that the pole masses extracted from the propagators in the symmetric phase agree well with the screening masses obtained recently in finite temperature SU(2) theory, while propagators measured in the broken phase show quite a different behaviour. T...
Heller UM, Karsch F, Rank J. The Gluon Propagator at High Temperature. Physics Letters B. 1995;355(3...
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 ...
Cucchieri A, Karsch F, Petreczky P. Screening in hot SU(2) gauge theory and propagators in 3d adjoin...
Karsch F, Neuhaus T, Patkos A, Rank J. Gauge boson masses in the 3D, SU(2) gauge-Higgs model. NUCLEA...
We investigate the large distance behavior of the electric and magnetic propagators of hot SU(2) gau...
We investigate the large distance behavior of the electric and magnetic propagators of hot SU(2) gau...
Cucchieri A, Karsch F, Petreczky P. Propagators and dimensional reduction of hot SU(2) gauge theory....
Heller UM, Karsch F, Rank J. Gluon propagator at high temperature: Screening, improvement and nonzer...
We study gauge boson propagators in the symmetric and symmetry broken phases of the 3-d, SU(2) gauge...
The screening masses of hot SU(N) gauge theory, defined as poles of the corresponding propagators ar...
We derive a set of gauge independent gap equations for Higgs boson and vector boson masses for the S...
KARKKAINEN L, LACOCK P, Miller D, Petersson B, REISZ T. THE PHYSICAL PHASE OF DIMENSIONALLY REDUCED ...
Kajantie K, Laine M, Rummukainen K, Shaposhnikov M. 3d SU(N) plus adjoint Higgs theory and finite-te...
Cucchieri A, Karsch F, Petreczky P. Magnetic screening in hot non-Abelian gauge theory. PHYSICS LETT...
Heller UM, Karsch F, Rank J. The Gluon Propagator at High Temperature. Physics Letters B. 1995;355(3...
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 ...
Cucchieri A, Karsch F, Petreczky P. Screening in hot SU(2) gauge theory and propagators in 3d adjoin...
Karsch F, Neuhaus T, Patkos A, Rank J. Gauge boson masses in the 3D, SU(2) gauge-Higgs model. NUCLEA...
We investigate the large distance behavior of the electric and magnetic propagators of hot SU(2) gau...
We investigate the large distance behavior of the electric and magnetic propagators of hot SU(2) gau...
Cucchieri A, Karsch F, Petreczky P. Propagators and dimensional reduction of hot SU(2) gauge theory....
Heller UM, Karsch F, Rank J. Gluon propagator at high temperature: Screening, improvement and nonzer...
We study gauge boson propagators in the symmetric and symmetry broken phases of the 3-d, SU(2) gauge...
The screening masses of hot SU(N) gauge theory, defined as poles of the corresponding propagators ar...
We derive a set of gauge independent gap equations for Higgs boson and vector boson masses for the S...
KARKKAINEN L, LACOCK P, Miller D, Petersson B, REISZ T. THE PHYSICAL PHASE OF DIMENSIONALLY REDUCED ...
Kajantie K, Laine M, Rummukainen K, Shaposhnikov M. 3d SU(N) plus adjoint Higgs theory and finite-te...
Cucchieri A, Karsch F, Petreczky P. Magnetic screening in hot non-Abelian gauge theory. PHYSICS LETT...
Heller UM, Karsch F, Rank J. The Gluon Propagator at High Temperature. Physics Letters B. 1995;355(3...
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 ...