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Rotating Melvin-like universes and wormholes in general relativity

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arxiv 2007.01145 v1 pith:QISOAX4Q submitted 2020-07-02 gr-qc hep-th

classification gr-qchep-th
keywords wormholemagneticaxiscurrentfieldsolutionscontaindescribe
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abstract

We find a family of exact solutions to the Einstein-Maxwell equations for rotating cylindrically symmetric distributions of a perfect fluid with the equation of state $p = w\rho$ ($|w| < 1$), carrying a circular electric current in the angular direction. This current creates a magnetic field along the $z$ axis. Some of the solutions describe geometries resembling that of Melvin's static magnetic universe and contain a regular symmetry axis, while some others (in the case $w > 0$) describe traversable wormhole geometries which do not contain a symmetry axis. Unlike Melvin's solution, those with rotation and a magnetic field cannot be vacuum and require a current. The wormhole solutions admit matching with flat-space regions on both sides of the throat, thus forming a cylindrical wormhole configuration potentially visible for distant observers residing in flat or weakly curved parts of space. The thin shells, located at junctions between the inner (wormhole) and outer (flat) regions, consist of matter satisfying the Weak Energy Condition under a proper choice of the free parameters of the model, and thus we obtain new examples of phantom-free wormhole models in general relativity. In the limit $w \to 1$, the magnetic field tends to zero, and the wormhole model tends to the one obtained previously, where the source of gravity is stiff matter with the equation of state $p = \rho$.

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  1. Gravitational lensing by Lema\^{\i}tre-Tolman-Bondi wormholes in a Friedmann universe

    gr-qc 2025-09 conditional novelty 6.0 of 10

    The angular size of a dust wormhole's shadow in a closed Friedmann universe first decreases, then increases with observation time, following a power-law relation in the wormhole size.

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