The microcanonical temperature is shown to be a useful concept in calculati
ons of the decay of a small isolated system with well defined energy. A sim
pler and more transparent description is obtained than in Klots' formulatio
n of finite-heat-bath theory, where the system is represented by a canonica
l ensemble. As a further illustration of the utility of the microcanonical
temperature concept, we discuss a formula derived by Dunbar for the probabi
lities for excitation of a single oscillator in a collection of harmonic os
cillators with well defined total energy. This formula expresses the excita
tion probabilities in terms of the temperature for a canonical ensemble wit
h mean energy equal to the energy of the system. However, a much improved a
ccuracy is obtained if the canonical temperature and heat capacity are repl
aced by their microcanonical values. We justify this replacement through a
modified derivation, in which the microcanonical temperature appears as the
canonical temperature of a fictitious system with level density rho'(E), t
he derivative of the level density rho (E) of the collection of oscillators
. (C) 2001 American Institute of Physics.