Finite Temperature LGT in a Finite Box with BPS Monopole Boundary Conditions

Details Finite Temperature LGT in a Finite Box with BPS Monopole Boundary Conditions Finite Temperature LGT in a Finite Box with BPS Monopole Boundary Conditions

1998-11-15

arxiv.org/abs/hep-lat/9811020v1

Nucl.Phys.Proc.Suppl. 73 (1999) 581-583

Physics

High Energy Physics

High Energy Physics - Lattice

LATTICE98(confine)

Scientific paper

10.1016/S0920-5632(99)85144-5

Finite temperature SU(2) lattice gauge theory is investigated in a 3D cubic box with fixed boundary conditions (b.c.) provided by a discretized, static BPS monopole solution with varying core scale ${\mu}$. For discrete ${\mu}$-values we find stable classical solutions either of electro-magnetic ('dyon') or of purely magnetic type inside the box. Near the deconfinement transition we study the influence of the b.c. on the quantized fields inside the box. In contrast to the purely magnetic background field case, for the dyon case we observe confinement for temperatures above the usual critical one.

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