The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs field of mass approximately 120 GeV, is examined to probe the crossover region between the symmetric and broken phase. Assuming the Higgs mass is constant, we find the width of this crossover region is approximately 20% of the average temperature. We suggest that this observable is a better parameter to explore this region of phase space than equal-time correlation functions, (C) 1998 Published by Elsevier Science B.V. All rights reserved
SUMMARY The Higgs SU(2) model with fixed Higgs length is usually believed to have two different ph...
Using lattice simulations we calculate the rate of baryon number violating processes, the sphaleron ...
We develop a topological method of measuring Chern-Simons number change in the real time evolution o...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
Karsch F, Laursen ML, Neuhaus T, Plache B. Fluctuations of Chern-Simons numbers in the SU(2) Higgs m...
Karsch F, Laurensen ML, Neuhaus T, Plache B. Thermal fluctuations of Chern-Simons numbers in the lat...
The rate of B-violation in the standard model at finite temperature is closely related to the diffus...
The Higgs SU(2) model with fixed Higgs length is usually believed to have two different phases at hi...
Karsch F, Laursen ML, Neuhaus T, Plache B. Chern-Simons term in the 4-dimensional SU(2) Higgs model....
SUMMARY The Higgs SU(2) model with fixed Higgs length is usually believed to have two different ph...
SUMMARY The Higgs SU(2) model with fixed Higgs length is usually believed to have two different ph...
Using lattice simulations we calculate the rate of baryon number violating processes, the sphaleron ...
We develop a topological method of measuring Chern-Simons number change in the real time evolution o...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
The classical transitions between topologically distinct vacua in a SU(2)-Higgs model, using a Higgs...
Karsch F, Laursen ML, Neuhaus T, Plache B. Fluctuations of Chern-Simons numbers in the SU(2) Higgs m...
Karsch F, Laurensen ML, Neuhaus T, Plache B. Thermal fluctuations of Chern-Simons numbers in the lat...
The rate of B-violation in the standard model at finite temperature is closely related to the diffus...
The Higgs SU(2) model with fixed Higgs length is usually believed to have two different phases at hi...
Karsch F, Laursen ML, Neuhaus T, Plache B. Chern-Simons term in the 4-dimensional SU(2) Higgs model....
SUMMARY The Higgs SU(2) model with fixed Higgs length is usually believed to have two different ph...
SUMMARY The Higgs SU(2) model with fixed Higgs length is usually believed to have two different ph...
Using lattice simulations we calculate the rate of baryon number violating processes, the sphaleron ...
We develop a topological method of measuring Chern-Simons number change in the real time evolution o...