Finite Systems in a Heat Bath: Spectrum Perturbations and Thermodynamics

When a finite system is at equilibrium with a heat bath, the equilibrium temperature is dictated by the heat bath and not by the intrinsic thermostatistics of the finite system. If not sufficiently large, it may be necessary for the finite system to change its thermostatistics in order to be at equilibrium with the heat bath. We account for this process by invoking Landsberg's notion of temperature-dependent energy levels. We establish that the mismatch between the intrinsic temperature of the excited finite system and that of the heat bath drives a spectrum perturbation which enables thermal equilibrium. We show that the temperature-induced spectrum perturbation is equivalent to Hill's purely thermodynamic subdivision potential. The difference between intrinsic and equilibrium temperature provides us with a measure for how large a system can be before it no longer needs to be regarded as small. The theoretical framework proposed in this paper identifies the role of temperature in a bottom-up thermostatistical description of finite systems.