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Radiatively induced spontaneous symmetry breaking and phase transitions in curved spacetime

Journal Article · · Ann. Phys. (N.Y.); (United States)
Local gauge symmetries which are spontaneously broken in flat spacetime are shown to be restored for large spactime curvatures. The case of symmetry breaking due to radiative quantum corrections in gauge theories with elementary scalar fields is considered explicity. In spacetimes with a postive Ricci curvature scalar R and a cosmological event horizon, the critical curvature R/sub C/ is of O(m/sub H/ /sup 2/) or O(m/sub w/ /sup 2/), depending on whether the theory is formulated with conformal or minimal scalar fields. In Ricci flat spacetimes with a conventional event horizon the symmetry is expected to be restored when the temperature of the Hawking thermal radiation is of O(m/sub w/). This phenomenon is described in detail, using functional integral methods and dimensional renormalization, for massless scalar electrodynamics in de-Sitter spacetime. For conformal scalars, the symmetry restoring phase transition is first order, the critical curvature being R/sub c/=0.910 m/sub H/ /sup 2/. For minimal scalars, an anomalous, curvature dependent mass counterterm is required. The phase transition in this case is second order, and occurs at R/sub C/=83.57 m/sub w/ /sup 2/. Symmetry restoration at finite temperature in flat spacetime is considered in an appendix. The critical temperature at which a first-order phase transition occurs in the Weinberg-Salam model is found to be T/sub C/=0.329 m/sub w/.
Research Organization:
Lyman Laboratory of Physics, Harvard University, Cambridge, Massachusetts 02138
OSTI ID:
6674873
Journal Information:
Ann. Phys. (N.Y.); (United States), Journal Name: Ann. Phys. (N.Y.); (United States) Vol. 128:2; ISSN APNYA
Country of Publication:
United States
Language:
English