The Berezinsky-Kosterlitz-Thouless (BKT) RG flow in the ensemble of monopoles existing in the finite-temperature (2+1)D Georgi-Glashow model is explored in the regime when the Higgs field is not infinitely heavy, but its mass is rather of the same order of magnitude as the mass of the W-boson. The corrections to the standard RG flow are derived to the leading order in the inverse mass of the Higgs boson. According to the obtained RG equations, the scaling of the free-energy density in the critical region and the value of the critical temperature of the phase transition are found to be unaffected by the finiteness of the Higgs-boson mass. The evolution of the Higgs mass itself is also investigated and shown to be rather weak, that enables on...
String representations of the Wilson loop and of the non-Abelian analog of the 't Hooft loop, define...
The renormalization-group equation for the zero-point energies associated with vacuum fluctuations o...
We study a chiral Yukawa model mimicking the Higgs–top–bottom sector of the standard model. We re-an...
The renormalization-group (RG) flow in the finite-temperature (2+1)-dimensional Georgi-Glashow model...
Confining strings and RG flow at finite temperature are investigated in the (2+1)-dimensional Georgi...
(2+1)-dimensional Georgi-Glashow model and its SU(N)-generalization are explored at nonzero temperat...
(2+1)-dimensional Georgi-Glashow model and its SU(N)-generalization are explored at nonzero temperat...
The (2+1)D Georgi-Glashow model is explored at finite temperature in the regime when the Higgs boson...
(2+1)-dimensional Georgi-Glashow model is explored in the regime when the Higgs boson is not infinit...
The (2+1)D Georgi-Glashow model is explored at finite temperature in the regime when the Higgs boson...
Confining strings are investigated in the (2+1)D Georgi-Glashow model. This is done in the limit whe...
(2+1)-dimensional Georgi-Glashow model, else called the Polyakov model, is explored at nonzero tempe...
We study the finite-temperature properties of the supersymmetric version of (2+1)D Georgi-Glashow mo...
It is shown that the SU(2) Higgs model on a lattice is equivalent to the Georgi--Glashow model in th...
Karsch F, Seiler E, Stamatescu IO. The SU(2) adjoint Higgs model at positive temperature: a Monte Ca...
String representations of the Wilson loop and of the non-Abelian analog of the 't Hooft loop, define...
The renormalization-group equation for the zero-point energies associated with vacuum fluctuations o...
We study a chiral Yukawa model mimicking the Higgs–top–bottom sector of the standard model. We re-an...
The renormalization-group (RG) flow in the finite-temperature (2+1)-dimensional Georgi-Glashow model...
Confining strings and RG flow at finite temperature are investigated in the (2+1)-dimensional Georgi...
(2+1)-dimensional Georgi-Glashow model and its SU(N)-generalization are explored at nonzero temperat...
(2+1)-dimensional Georgi-Glashow model and its SU(N)-generalization are explored at nonzero temperat...
The (2+1)D Georgi-Glashow model is explored at finite temperature in the regime when the Higgs boson...
(2+1)-dimensional Georgi-Glashow model is explored in the regime when the Higgs boson is not infinit...
The (2+1)D Georgi-Glashow model is explored at finite temperature in the regime when the Higgs boson...
Confining strings are investigated in the (2+1)D Georgi-Glashow model. This is done in the limit whe...
(2+1)-dimensional Georgi-Glashow model, else called the Polyakov model, is explored at nonzero tempe...
We study the finite-temperature properties of the supersymmetric version of (2+1)D Georgi-Glashow mo...
It is shown that the SU(2) Higgs model on a lattice is equivalent to the Georgi--Glashow model in th...
Karsch F, Seiler E, Stamatescu IO. The SU(2) adjoint Higgs model at positive temperature: a Monte Ca...
String representations of the Wilson loop and of the non-Abelian analog of the 't Hooft loop, define...
The renormalization-group equation for the zero-point energies associated with vacuum fluctuations o...
We study a chiral Yukawa model mimicking the Higgs–top–bottom sector of the standard model. We re-an...