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Probing Chaos in Schwarzschild-de Sitter Spacetime: The Role of Black Hole and Cosmological Horizons

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arxiv 2502.12758 v1 pith:DXDUHIUE submitted 2025-02-18 gr-qc hep-thnlin.CD

Probing Chaos in Schwarzschild-de Sitter Spacetime: The Role of Black Hole and Cosmological Horizons

classification gr-qc hep-thnlin.CD
keywords chaoshorizonssystemlyapunovspacetimeblackchaoticcosmological
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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In this paper, we study the motion of a massless, chargeless particle in Schwarzschild-de Sitter spacetime, revealing exponential radial growth and potential chaos in an integrable system. Poincar\'e sections show regular Kolmogorov-Arnold-Moser (KAM) tori when black hole and cosmological horizons are distant, but distortions and chaos emerge as they converge. As the horizons coincide, the Poincar\'e sections fully contract and vanish, marking the system's transition to Nariai spacetime. \textit{Our analysis also suggests that, within the parameter range explored, the event horizon exerts a comparatively more substantial chaotic influence on the system, primarily due to its consistent proximity.} Additionally, we analyze the Lyapunov exponents to quantify the degree of chaos in the system. Our findings indicate that as the closeness of the two horizons increases, the most prominent Lyapunov exponent also increases, signifying a rise in chaotic behavior. By examining the long-term saturation values of the Lyapunov exponents, we confirm that they consistently comply with the Maldacena-Shenker-Stanford (MSS) bound.

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  1. Discussion on the equivalence of two relativistic point-particle Lagrangians

    gr-qc 2026-04 unverdicted novelty 6.0

    The Lagrangians L1 = -mc sqrt(-g dot x dot x) - V and L2 = (1/2)m g dot x dot x - V are equivalent only for V=0 or electromagnetic V; otherwise L1 enforces mass shell while L2 does not, leading to chaotic vs integrabl...