Randomized trial analyzes black hole models in cosmological context, suggesting new insights into general relativity.
The Cosmological General Theory of Relativity (CGTR) extends the Cosmological Special Theory of Relativity (CSTR) to curved spacetime byembedding a localized mass, or a rotating charged mass, within a spatially flat, spatially homogeneous Robertson-Walker background whosescale factor is denoted the cosmological expansion function τ (t0) (Yi, 2020, 2021). This paper concentrates specifically on the black-holesolutions of this framework: the cosmologically embedded Schwarzschild solution and the cosmologically embedded Kerr-Newman solution(Yi, 2021, 2025). We present the CGTR field equation and its perturbative metric ansatz, derive the Schwarzschild and Kerr-Newman metricfunctions and their horizon structure, work out the radial and circular photon and massive-particle geodesics, the ergosphere and extremalitycondition of the rotating solution, and the homogeneous (source-free) limit that recovers the background Robertson-Walker cosmology.We show that, in every case considered, the physically measured horizon radii, extremality condition, and photon-sphere radius reduce totheir ordinary, epoch-independent general-relativistic values once expressed in the physically expanded radial coordinate, even though thecorresponding local-coordinate expressions carry explicit τ (t0)-dependence. We close with a comparison to the mainstream McVittie andSchwarzschild-de Sitter embeddings of a point mass in an expanding or accelerating universe, and with the open questions raised by anindependent critical review of the underlying CSTR framework (A Critical Review, 2025).
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Sangwha Yi (2026) studied this question.
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