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Exact regular black hole solutions with de Sitter cores and Hagedorn fluid

Vitalii VertogradovPhysics Department, Herzen State Pedagogical University of Russia, 48 Moika Emb., Saint Petersburg 191186, RussiaAli ÖvgünPhysics Department, Eastern Mediterranean University, via Mersin 10, Famagusta 99628, North Cyprus, Turkey
2024en
ABI

Аннотация

Abstract In this paper, we present three exact solutions to the Einstein field equations, each illustrating different black hole models. The first solution introduces a black hole with a variable equation of state, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>P</mml:mi> <mml:mo>=</mml:mo> <mml:mi>k</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>r</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:mi>ρ</mml:mi> </mml:mrow> </mml:math> , which can represent both singular and regular black holes depending on the parameters M 0 and w 0 . The second solution features a black hole with Hagedorn fluid, relevant to the late stages of black hole formation, and reveals similarities to the first solution by also describing both singular and regular black holes in a specific case. Furthermore, we investigate the shadows cast by these black hole solutions to constrain their parameters. Recognizing that real astrophysical black holes are dynamic, we developed a third, dynamical solution that addresses gravitational collapse and suggests the potential formation of naked singularities. This indicates that a black hole can transition from regular to singular and back to regular during its evolution.

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