Abstract

In the previous paper, we have shown the existence of magnetic monopoles in the pure SU(2) Yang–Mills theory with a gauge-invariant mass term for the gluon field being introduced. In this paper, we extend our previous construction of magnetic monopoles to obtain dyons with both magnetic and electric charges. In fact, we solve under the static and spherically symmetric ansatz the field equations of the SU(2) “complementary” gauge-scalar model, which is the SU(2) Yang–Mills theory coupled to a single adjoint scalar field whose radial degree of freedom is eliminated. We show that the novel dyon solution can be identified with the gauge field configuration of a dyon with a minimum magnetic charge in the massive Yang–Mills theory. Moreover, we compare the dyon of the massive Yang–Mills theory obtained in this way with the Julia–Zee dyon in the Georgi–Glashow gauge-Higgs scalar model and the dyonic extension of the Wu–Yang magnetic monopole in the pure Yang–Mills theory. Finally, we identify the novel dyon solution found in this paper with a dyon configuration on S^1 times {mathbb {R}}^3 space with nontrivial holonomy and propose to use it to understand the confinement/deconfinement phase transition in the Yang–Mills theory at finite temperature, instead of using the dyons constituting the Kraan–van Baal–Lee–Lu caloron.

Highlights

  • Hooft–Polyakov magnetic monopole [4,5,6] exists as a topological soliton solution of the field equations of the Georgi– Glashow gauge-Higgs scalar model in which a single scalar field belongs to the adjoint representation of the gauge group SU (2)

  • The procedure for obtaining the relevant dyon is guided by the “complementarity” between the SU (2) gauge-adjoint scalar model with a single radially fixed scalar field and the massive SU (2) Yang–Mills theory

  • We have found that the static energy or the rest mass of the obtained Yang–Mills dyon is finite and proportional to the mass MX of the Yang–Mills gauge field A representing the existence of the massive component X

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Summary

Introduction

Hooft–Polyakov magnetic monopole [4,5,6] exists as a topological soliton solution of the field equations of the Georgi– Glashow gauge-Higgs scalar model in which a single scalar field belongs to the adjoint representation of the gauge group SU (2). We review the procedure [9] for obtaining the massive SU (2) Yang–Mills theory from the “complementary” SU (2) gauge-adjoint scalar model For this purpose, we introduce the two products for the Lie-algebra valued fields P := P ATA and Q = QATA ( A = 1, 2, 3):. We can observe that the theory with the new field variables has two extra degrees of freedom if we wish to obtain the (pure) Yang–Mills theory from the “complementary” gauge-scalar model. We write the vacuum-to-vacuum amplitude of the gauge-scalar model subject to the reduction condition translated into the massive Yang–Mills theory with the gauge-invariant mass term of the field X as.

Julia–Zee dyon solution in the Georgi–Glashow model
Construction of the Yang–Mills dyon
Gauge field decomposition for a dyon
Chromoelectric and chromomagnetic fields of a dyon
Energy density and static mass of a dyon
The self-dual dyon and the KvBLL caloron in the massless Yang–Mills theory
Conclusion and discussion
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