Caloric curve of star clusters

TL;DR

This paper investigates how a short-distance cutoff in the King model of globular clusters influences the caloric curve, revealing stabilization of a low-energy phase and similarities to other regularized models.

Contribution

It introduces a modified King model with a short-distance cutoff and analyzes its impact on the caloric curve, providing insights into the thermodynamics of self-gravitating systems.

Findings

The cutoff stabilizes a low-energy phase absent in the uncut model.

The caloric curve resembles that of other regularized models, lacking a high-energy gas phase.

Results have implications for understanding the thermodynamics of real self-gravitating systems.

Abstract

Self-gravitating systems, like globular clusters or elliptical galaxies, are the prototypes of many-body systems with long-range interactions, and should be the natural arena where to test theoretical predictions on the statistical behaviour of long-range-interacting systems. Systems of classical self-gravitating particles can be studied with the standard tools of equilibrium statistical mechanics, provided the potential is regularized at small length scales and the system is confined in a box. The confinement condition looks rather unphysical in general, so that it is natural to ask whether what we learn with these studies is relevant to real self-gravitating systems. In order to provide a first answer to this question we consider a basic, simple, yet effective model of globular clusters, the King model. This model describes a self-consistently confined system, without the need of any external box, but the stationary state is a non-thermal one. In particular, we consider the King model with a short-distance cutoff on the interactions and we discuss how such a cutoff affects the caloric curve, i.e. the relation between temperature and energy. We find that the cutoff stabilizes a low-energy phase which is absent in the King model without cutoff; the caloric curve of the model with cutoff turns out to be very similar to that of previously studied confined and regularized models, but for the absence of a high-energy gas-like phase. We briefly discuss the possible phenomenological as well as theoretical implications of these results.