Journal
JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 1, Pages -Publisher
SPRINGER
DOI: 10.1007/JHEP01(2021)166
Keywords
Classical Theories of Gravity; Solitons Monopoles and Instantons; Spontaneous Symmetry Breaking
Categories
Funding
- National Science and Engineering Research Council of Canada (NSERC)
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This paper numerically finds static vortex solutions under Einstein gravity in an AdS(3) background, where the scalar and gauge fields have a non-singular profile and positive mass without an event horizon. The mass of the vortex increases as the cosmological constant becomes more negative, leading to a smaller core. Additionally, the study explores vortex solutions with and without gravity in asymptotically flat spacetime, revealing novel possibilities for gravitational potential in General Relativity supplemented with scalar fields.
In previous work, black hole vortex solutions in Einstein gravity with AdS(3) background were found where the scalar matter profile had a singularity at the origin r = 0. In this paper, we find numerically static vortex solutions where the scalar and gauge fields have a non-singular profile under Einstein gravity in an AdS(3) background. Vortices with different winding numbers n, VEV v and cosmological constant Lambda are obtained. These vortices have positive mass and are not BTZ black holes as they have no event horizon. The mass is determined in two ways: by subtracting the numerical values of two separate asymptotic metrics and via an integral that is purely over the matter fields. The mass of the vortex increases as the cosmological constant becomes more negative and this coincides with the core of the vortex becoming smaller (compressed). We then consider the vortex with gravity in asymptotically flat spacetime for different values of the coupling alpha = 1/(16 pi G). At the origin, the spacetime has its highest curvature and there is no singularity. It transitions to an asymptotic conical spacetime with angular deficit that increases significantly as alpha decreases. For comparison, we also consider the vortex without gravity in flat spacetime. For this case, one cannot obtain the mass by the first method (subtracting two metrics) but remarkably, via a limiting procedure, one can obtain an integral mass formula. In the absence of gauge fields, there is a well-known logarithmic divergence in the energy of the vortex. With gravity, we present this divergence in a new light. We show that the metric acquires a logarithmic term which is the 2 + 1 dimensional realization of the Newtonian gravitational potential when General Relativity is supplemented with a scalar field. This opens up novel possibilities which we discuss in the conclusion.
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