1994
DOI: 10.1103/physrevd.50.4162
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Spherical shells of a classical gauge field and their topological charge as a perturbative expansion

Abstract: We consider the classical equations of motion of SU (2) gauge theory, without a Higgs field, in Minkowski space. We work in the spherical ansatz and develop a perturbative expansion in the coupling constant g for solutions which in the far past look like freely propagating spherical shells. The topological charge Q of these solutions is typically non-integer. We then show that Q can be expressed as a power series expansion in g which can be nonzero at finite order. We give an explicit analytic calculation of t… Show more

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Cited by 8 publications
(38 citation statements)
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“…The classical evolution of certain gauge field configurations in Minkowski space was addressed in Refs. [7][8]. In this paper we study fermion number violation in the background of a gauge field in Minkowski space.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The classical evolution of certain gauge field configurations in Minkowski space was addressed in Refs. [7][8]. In this paper we study fermion number violation in the background of a gauge field in Minkowski space.…”
Section: Introductionmentioning
confidence: 99%
“…On classical solutions in Minkowski space Q in general can take any value, not just an integer [7,8]. This is a consequence of the fact that classical Minkowski gauge fields do not approach just some pure gauges in the far past and future, but the finite energy radiation is always present.…”
Section: Introductionmentioning
confidence: 99%
“…In a companion paper 9 we analyze fermion production in the background of a field which locally changes winding number. We work with a (1+1)-dimensional analogue.…”
Section: Discussionmentioning
confidence: 99%
“…In a companion paper 9 we study fermion number production in a (1+1)-dimensional theory with an arbitrary background gauge field. We arrange for the background field to change its winding number in local regions and we allow for these local changes to be non-integer.…”
mentioning
confidence: 99%
“…First, we write the complex fields χ and φ in polar form 1 1 In Ref. [3] the phase of χ was called ϕ. In this paper we call it θ.…”
Section: Gauge Invariant Variablesmentioning
confidence: 99%