Jeans analysis of self-gravitating systems inf(R)gravity
[EN]Dynamics and collapse of collisionless self-gravitating systems is described by the coupled collisionless Boltzmann and Poisson equations derived from f(R) gravity in the weak field approximation. Specifically, we describe a system at equilibrium by a time-independent distribution function f0(x,...
| Autores: | , , , , |
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| Tipo de recurso: | artículo |
| Estado: | Versión publicada |
| Fecha de publicación: | 2012 |
| País: | España |
| Institución: | Universidad de Salamanca (USAL) |
| Repositorio: | GREDOS. Repositorio Institucional de la Universidad de Salamanca |
| OAI Identifier: | oai:gredos.usal.es:10366/155240 |
| Acceso en línea: | http://hdl.handle.net/10366/155240 |
| Access Level: | acceso abierto |
| Palabra clave: | Post-Newtonian approximation Modified theories of gravity General Relativity and Quantum Cosmology Astrophysics - High Energy Astrophysical Phenomena |
| Sumario: | [EN]Dynamics and collapse of collisionless self-gravitating systems is described by the coupled collisionless Boltzmann and Poisson equations derived from f(R) gravity in the weak field approximation. Specifically, we describe a system at equilibrium by a time-independent distribution function f0(x,v) and two potentials Φ0(x) and Ψ0(x) solutions of the modified Poisson and collisionless Boltzmann equations. Considering a small perturbation from the equilibrium and linearizing the field equations, it can be obtained a dispersion relation. A dispersion equation is achieved for neutral dust-particle systems where a generalized Jeans wave number is obtained. This analysis gives rise to unstable modes not present in the standard Jeans analysis (derived assuming Newtonian gravity as weak filed limit of f(R)=R). In this perspective, we discuss several self-gravitating astrophysical systems whose dynamics could be fully addressed in the framework of f(R) gravity. |
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