Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations of a collisionless Maxwell-Boltzmann gas with nonstandard self- interactions, modeled by an effective one-particle force. The resulting set of equilibrium conditions represents a generalization of the classical Tolman-Oppenheimer-Volkov equations. We specify these conditions for two types of Lorentz-like forces: one coupled to the 4-acceleration and the 4-velocity and the other one coupled to the Riemann tensor. We investigate the weak field limits in each case and show that they lead to various Newtonian type configurations that are different from the usual isothermal sphere characterizing the conventional Newtonian Maxwell-Boltzmann gas. T...
We show that a relativistic gas may be at "global" equilibrium in the expanding universe for any equ...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
We consider simple hydrodynamical models of galactic dark matter in which the galactic halo is a sel...
We provide a general framework for self-interacting warm dark matter (WDM) in cosmological perturbat...
We consider simple hydrodynamical models of galactic dark matter in which the galactic halo is a sel...
After deducing the density profiles and gravitational potential functions of eight galaxies from the...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
We provide a general framework for self-interacting warm dark matter (WDM) in cosmological perturbat...
We show that a relativistic gas may be at "global" equilibrium in the expanding universe for any equ...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
Using relativistic kinetic theory, we study spherically symmetric, static equilibrium configurations...
We consider simple hydrodynamical models of galactic dark matter in which the galactic halo is a sel...
We provide a general framework for self-interacting warm dark matter (WDM) in cosmological perturbat...
We consider simple hydrodynamical models of galactic dark matter in which the galactic halo is a sel...
After deducing the density profiles and gravitational potential functions of eight galaxies from the...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
International audienceWe consider models of scalar dark matter with a generic interaction potential ...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
We provide a general framework for self-interacting warm dark matter (WDM) in cosmological perturbat...
We show that a relativistic gas may be at "global" equilibrium in the expanding universe for any equ...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...
The particles of a classical relativistic gas are assumed to move under the influence of a quasiline...