4.7 Article

Gravitating superconducting solitons in the (3+1)-dimensional Einstein gauged non-linear σ-model

Journal

EUROPEAN PHYSICAL JOURNAL C
Volume 81, Issue 1, Pages -

Publisher

SPRINGER
DOI: 10.1140/epjc/s10052-021-08854-x

Keywords

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Funding

  1. Fondecyt [1200022, 1200293]
  2. Chilean Government through the Centers of Excellence Base Financing Program of Conicyt
  3. National Research Foundation of Korea - Ministry of Education of Korea [2018-R1D1A1B0-7048945, 2017-R1A2B4010738]
  4. FONDECYT-post-doctoral grant [3190873, 3200884]

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This paper presents the first analytic examples of (3+1) -dimensional self-gravitating regular cosmic tube solutions which are superconducting and free of curvature singularities. The solutions resemble a boosted cosmic string with an angular defect at large distances from the axis, and near the axis, they can be singularity free. The solutions can behave as superconductors and carry a persistent current tied to their topological charge.
In this paper, we construct the first analytic examples of (3+1) -dimensional self-gravitating regular cosmic tube solutions which are superconducting, free of curvature singularities and with non-trivial topological charge in the Einstein-SU(2) non-linear sigma -model. These gravitating topological solitons at a large distance from the axis look like a (boosted) cosmic string with an angular defect given by the parameters of the theory, and near the axis, the parameters of the solutions can be chosen so that the metric is singularity free and without angular defect. The curvature is concentrated on a tube around the axis. These solutions are similar to the Cohen-Kaplan global string but regular everywhere, and the non-linear sigma -model regularizes the gravitating global string in a similar way as a non-Abelian field regularizes the Dirac monopole. Also, these solutions can be promoted to those of the fully coupled Einstein-Maxwell non-linear sigma -model in which the non-linear sigma -model is minimally coupled both to the U(1) gauge field and to General Relativity. The analysis shows that these solutions behave as superconductors as they carry a persistent current even when the U(1) field vanishes. Such persistent current cannot be continuously deformed to zero as it is tied to the topological charge of the solutions themselves. The peculiar features of the gravitational lensing of these gravitating solitons are shortly discussed.

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