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Scientific Report 2007-2009<br />

Astronomy & Astrophysics<br />

A4. Equilibrium and stability of relativistic stellar clusters and study<br />

of properties of systems with anisotropic distribution of stars<br />

velocities<br />

The study of compact objects like relativistic stellar<br />

clusters is considered one of the most important topics<br />

in General Relativity, being the collapse of dense stellar<br />

cluster one of the possible ways of formation of supermassive<br />

black holes in quasars and galactic nuclei. The<br />

structure and stability of such systems is strongly depending<br />

on energy cutoff which takes into account the<br />

evaporation of stars with large velocity. Also anisotropy<br />

in momentum space may appear during the possible<br />

rapid contraction of the cluster due to the preservation<br />

of angular momentum. Strong anisotropy is expected<br />

in dense clusters with a supermassive black hole at the<br />

center, where in the vicinity of the last stable orbit only<br />

stars with circular orbits can survive.<br />

The study of the equilibrium configurations and their<br />

dynamic and thermodynamic stability for clusters has<br />

been systematically and deeply managed by constructing<br />

non collisional selfgravitating models with spherical symmetry<br />

and distribution function with a velocity cutoff.<br />

Stability of isotropic clusters is analyzed by constructing<br />

appropriate sequences of models by varying suitable<br />

parameters. Results of this analysis lead to conclusion<br />

that equilibrium configurations are dynamically stable in<br />

Newtonian regime, independently from the choice of distribution<br />

function while, in relativistic regime, a critical<br />

density showing the appearance of dynamical instabilities<br />

has been obtained. The general analysis of thermodynamical<br />

and dynamical stability can be performed by<br />

constructing a z c − T diagram of the equilibrium configuration<br />

(see Figure 1).<br />

of dynamical and thermodynamical instability for large<br />

values of temperature T [2]. Perspectives of this research<br />

is extending this analysis to anisotropic models. With<br />

the study of the equilibrium models with anisotropic distribution<br />

it is possible to see that these systems mantain<br />

the spherical symmetry if the total angular momentum<br />

is zero. The main characteristic of these models is the<br />

appearance of a hollow structure for which the density<br />

profile shows an increasing behavior at increasing values<br />

of radius at sufficiently large level of anisotropy [1,3].<br />

The study of thermodynamical instabilities of selfgravitating<br />

systems is strictly connected with the problem of<br />

gravothermal cathastrophe first introduced by the well<br />

known paper of Lynden-Bell & Wood in 1968. In this<br />

model, the effect of the presence of region at negative<br />

thermal capacity leads the system towards the collapse of<br />

the core. The rough picture introduced by Lynden-Bell<br />

& Wood has been developed by constructing a selfconsistent<br />

model in which regions at negative thermal capacity<br />

coexists with positive ones (see Figure 2) on the basis of<br />

the application of statistical mechanics in presence of<br />

gravity. The general properties of these models are well<br />

fitting the main characteristics of globular clusters, by<br />

using the King distribution function, and give the possibility<br />

to analyze the dynamical evolution of the systems<br />

until the onset of the gravothermal catastrophe.<br />

1<br />

0.8<br />

0.6<br />

W0=5.0<br />

0.4<br />

W0=3.5<br />

thermodynamic onset<br />

dynamic onset<br />

(Cv/Nk)r<br />

W0=2.0<br />

0.2<br />

W0=1.35<br />

10 1 with<br />

dynamically<br />

stable<br />

configurations<br />

unstable configurations<br />

0<br />

W0=0.8<br />

-0.2<br />

z c<br />

10 0<br />

thermodynamical<br />

instability<br />

-0.4<br />

-0.6<br />

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1<br />

r/R<br />

stable configurations<br />

10 -1<br />

10 -2 10 -1 10 0 10 1<br />

Figure 1: Regions of dynamical and thermodynamical stability<br />

in the plane (T, z c).<br />

The main result is the existence of dynamically stable<br />

solutions for arbitrarily large values of the central<br />

redshift z c for sufficiently small values of the temperature<br />

T and the contemporary appearance of the onset<br />

T<br />

Figure 2: Values of thermal capacity in Nk units as a function<br />

of relative radius r/R for selected values of central potential<br />

W 0 .<br />

References<br />

1. G.S. Bisnovatyi-Kogan et al., ApJ 703, 628 (2009).<br />

2. M. Merafina et al., AIP, 1206, 399 (2009).<br />

3. G.S. Bisnovatyi-Kogan et al., ApJ,<br />

Authors<br />

M. Merafina<br />

<strong>Sapienza</strong> Università di Roma 151 Dipartimento di Fisica

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