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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