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Black Hole Solutions in Non-Minimally Coupled Weyl Connection Gravity

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arxiv 2410.01856 v2 pith:C6JXXYCY submitted 2024-10-02 gr-qc hep-th

classification gr-qchep-th
keywords solutionsconstantcosmologicalblackcurvatureholemattervacuum
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abstract

Schwarzschild and Reissner-Nordstr{\o}m black hole solutions are found in the context of a non-minimal matter-curvature coupling with the Weyl connection, both in vacuum and in the presence of a cosmological constant-like matter content. This special case of non-metricity leads to black hole solutions with non-vanishing scalar curvature. Moreover, vacuum Schwarzschild solutions differ from the ones from a constant curvature scenario in $f(R)$ theories with the appearance of a coefficient in the term linear in r and a corrected "cosmological constant". Non-vacuum Shwarzschild solutions have formally the same solutions as in the previous case with the exception being the physical interpretation of a cosmological constant as the source of the matter Lagrangian as not a simple reparametrization of the $f(R)$ description. Reissner-Nordstr{\o}m solutions cannot be found in vacuum, but only in the presence of matter fields, such that the solutions also differ from the constant curvature scenario in $f(R)$ theories by the term linear in r and corrected/dressed charge and cosmological constant.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Atomic clocks and gravitational waves as probes of non-metricity

    gr-qc 2026-01 reject novelty 5.0 of 10

    The paper claims existing gravitational-wave data already bound Weyl non-metricity, α²ω̄0<10⁻⁶⁹ GeV, via backreaction of a Planck-scale Weyl field, but a dropped kinetic term numerically exceeds the assumed sensitivity.

  2. Weak Field Limit of the Nonminimally Coupled Weyl Connection Gravity

    gr-qc 2025-06 reject novelty 5.0 of 10

    The weak-field limit of nonminimally coupled Weyl connection gravity is claimed to yield explicit equations for the Bardeen potentials and the Weyl vector, but the key step is algebraically inconsistent.

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