Dynamics of non-integrable phases and gauge symmetry breaking
On a multiply-connected space the non-integrable phase factor/ital P/ exp(ig..integral../ital A//sub ..mu..//ital dx//sup ..mu..//r brace/), a path-ordered line integral along anon-contractable loop, becomes a dynamical degree of freedom in gauge theory.The dynamics of such non-integrable phases are examined in detail with themost general boundary condition for gauge fields and fermions. Sometimesthe dynamics of the non-integrable phases compensate the arbitrariness inthe boundary condition imposed, leading to the same physics results. Inother cases the dynamics of the non-integrable phases induce spontaneousbreaking of non-Abelian gauge symmetry. In other words the physically realizedsymmetry of the system differs from, and can be either greater or smaller than,the symmetry of the boundary condition. The effective potential for thenon-integrable phases in the /ital SU/(/ital N/) gauge theory on/ital S//sup 1//direct product//ital R//sup 1/ital d//minus/2/is computed in the one-loop approximation. It is shown that the gauge symmetryis dynamically broken in the presence of fermions in the adjoint representation,depending on the value of the boundary condition parameter./copyright/ 1989 Academic Press, Inc.
- Research Organization:
- School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455(US)
- OSTI ID:
- 6391277
- Journal Information:
- Ann. Phys. (N.Y.); (United States), Vol. 190:2
- Country of Publication:
- United States
- Language:
- English
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645400* - High Energy Physics- Field Theory