Stationary Stars Are Axisymmetric in Higher Curvature Gravity
arXiv:2512.10343 · doi:10.1103/n8xm-6s3v
Abstract
The final equilibrium stage of stellar evolution can result in either a black hole or a compact object such as a white dwarf or neutron star. In general relativity, both stationary black holes and stationary stellar configurations are known to be axisymmetric, and black hole rigidity has been extended to several higher curvature modifications of gravity. In contrast, no comparable result had previously been established for stationary stars beyond general relativity. In this work we extend the stellar axisymmetry theorem to a broad class of diffeomorphism invariant metric theories. Assuming asymptotic flatness and standard smoothness requirements, we show that the Killing symmetry implied by thermodynamic equilibrium inside the star uniquely extends to the exterior region, thereby enforcing rotational invariance. This demonstrates that axisymmetry of stationary stellar configurations is not a feature peculiar to Einstein gravity but a universal property of generally covariant gravitational theories, persisting even in the presence of higher curvature corrections.
arXiv comment14 pages, accepted in PRD
References in corpus (13)
- Some Properties of Noether Charge and a Proposal for Dynamical Black Hole Entropy
- A Note on Thermodynamics of Black Holes in Lovelock Gravity
- Lanczos-Lovelock models of gravity
- Brane versus shell cosmologies in Einstein and Einstein-Gauss-Bonnet theories
- Well-posed formulation of Lovelock and Horndeski theories
- On the local well-posedness of Lovelock and Horndeski theories
- Entropy increase during physical processes for black holes in Lanczos-Lovelock gravity
- Black Hole Thermodynamics: General Relativity and Beyond
- Shock Formation in Lovelock Theories
- Black Hole Zeroth Law in Higher Curvature Gravity
- Intersecting hypersurfaces, topological densities and Lovelock Gravity
- A stationary black hole must be axisymmetric in effective field theory
- Thin shell dynamics in Lovelock gravity