paper

The non-minimally coupled gravitating vortex: phase transition at critical coupling in AdS

arXiv:2205.12175 · doi:10.1103/PhysRevD.106.065017

Abstract

We consider the Nielsen-Olesen vortex non-minimally coupled to Einstein gravity with cosmological constant . A non-minimal coupling term is natural to add to the vortex as it preserves gauge-invariance (here is the Ricci scalar and a dimensionless coupling constant). This term plays a dual role: it contributes to the potential of the scalar field and to the Einstein-Hilbert term for gravity. As a consequence, the vacuum expectation value (VEV) of the scalar field and the cosmological constant in the AdS background depend on . This leads to a novel feature: there is a critical coupling where the VEV is zero for but becomes non-zero when crosses below and the gauge symmetry is spontaneously broken. Moreover, we show that the VEV near the critical coupling has a power law behaviour proportional to . Therefore can be viewed as the analog of the critical temperature in Ginzburg-Landau (GL) mean-field theory where a second-order phase transition occurs below and the order parameter has a similar power law behaviour near . The critical coupling exists only in an AdS background; it does not exist in asymptotically flat spacetime (topologically a cone) where the VEV remains at a fixed non-zero value independent of . However, the deficit angle of the asymptotic conical spacetime depends on and is no longer determined solely by the mass; remarkably, a higher mass does not necessarily yield a higher deficit angle. The equations of motion are more complicated with the non-minimal coupling term present. However, via a convenient substitution one can reduce the number of equations and solve them numerically to obtain exact vortex solutions.

50 pages, 21 figures, two tables. v2: version to appear in PRD

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