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Phys. Rev. D 19, 3682–3697 (1979)

Phase diagrams of lattice gauge theories with Higgs fields

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Eduardo Fradkin
Stanford Linear Accelerator Center, Stanford University, Stanford, California 94305 and Physics Department, Stanford University, Stanford, California 94305

Stephen H. Shenker
Laboratory of Nuclear Studies, Cornell University, Ithaca, New York 14853

Received 18 January 1979; published in the issue dated 15 June 1979

We study the phase diagram of lattice gauge theories coupled to fixed-length scalar (Higgs) fields. We consider several gauge groups: Z2, U(1), and SU(N). We find that when the Higgs fields transform like the fundamental representation of the gauge group the Higgs and confining phases are smoothly connected, i.e., they are not separated by a phase boundary. When the Higgs fields transform like some representation other than the fundamental, a phase boundary may exist. This is the case for SU(N) with all the Higgs fields in the adjoint representation and for U(1) with all the Higgs fields in the charge-N(N>1) representation. We present an argument due to Wegner that indicates the stability of the pure gauge transition. Another phase, free charge or Coulomb, is generally present. In this regime, the spectrum of the theory contains massless gauge bosons (for continuous groups) and finite-energy states that represent free charges.

© 1979 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.19.3682
DOI:
10.1103/PhysRevD.19.3682
PACS: