1974
DOI: 10.1103/physrevd.10.4138
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Nonperturbative methods and extended-hadron models in field theory. III. Four-dimensional non-Abelian models

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Cited by 240 publications
(174 citation statements)
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“…Monopoles are essentially related to the presence of the Higgs field with the SO(3) component, while for sphalerons Higgs can be replaced by other attractive agent. Recall that the sphaleron was first obtained in the gauge theory with doublet Higgs [19] and its existence was explained by Manton [20] as a consequence of non-triviality of the third homotopy group of the broken phase manifold. Later it was found that similar solutions arise in the theories without Higgs like Einstein-Yang-Mills and Yang-Mills with dilaton (for a review see [21]), in all such cases conformal invariance is broken.…”
Section: Glueballsmentioning
confidence: 99%
See 1 more Smart Citation
“…Monopoles are essentially related to the presence of the Higgs field with the SO(3) component, while for sphalerons Higgs can be replaced by other attractive agent. Recall that the sphaleron was first obtained in the gauge theory with doublet Higgs [19] and its existence was explained by Manton [20] as a consequence of non-triviality of the third homotopy group of the broken phase manifold. Later it was found that similar solutions arise in the theories without Higgs like Einstein-Yang-Mills and Yang-Mills with dilaton (for a review see [21]), in all such cases conformal invariance is broken.…”
Section: Glueballsmentioning
confidence: 99%
“…1. The integer n is equal to the number of zeroes of w. The n = 1 solution is an analog of the sphaleron known in the Weinberg-Salam theory [19,20], it is expected to have one decay mode. Higher odd-n solutions may be interpreted as excited sphalerons, they Fig.…”
Section: Glueballsmentioning
confidence: 99%
“…In fact, in the absence of the hypercharge U(1) degrees of freedom, the above ansatz describes the SU(2) sphaleron which is not spherically symmetric [6]. The situation changes with the inclusion of the extra hypercharge U(1) in the standard model, which can compensate the action of the U(1) subgroup of SU (2) on the Higgs field.…”
mentioning
confidence: 99%
“…However, there exists a static unstable solution of the field equations, known as sphaleron [3][4][5][6], that represents the top of the energy barrier between two distinct vacua and at finite temperature, because of thermal fluctuations of fields, fermion number violating vacuum to vacuum transitions can occur which are only suppressed by a Boltzmann factor, containing the height of the barrier at the given temperature, i.e. the energy of the sphaleron [7].…”
Section: Introductionmentioning
confidence: 99%