Physics – High Energy Physics – High Energy Physics - Phenomenology
Scientific paper
2003-06-22
Mod.Phys.Lett. A18 (2003) 2873-2886
Physics
High Energy Physics
High Energy Physics - Phenomenology
one error is corrected
Scientific paper
10.1142/S0217732303012441
The well known topological monopoles originally investigated by 't Hooft and Polyakov are known to arise in classical Yang-Mills-Higgs theory. With a pure gauge theory it is known that the classical Yang-Mills field equation do not have such finite energy configurations. Here we argue that such configurations may arise in a semi-quantized Yang-Mills theory, where the original gauge group, SU(3), is reduced to a smaller gauge group, SU(2), and with some combination of the coset fields of the SU(3) to SU(2) reduction acting as effective scalar fields. The procedure is called semi-quantized since some of the original gauge fields are treated as quantum degrees of freedom, while others are postulated to be effectively described as classical degrees of freedom. Some speculation is offer on a possible connection between these monopole configurations and the confinement problem, and the nucleon spin puzzle.
Dzhunushaliev Vladimir
Singleton Doug
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