Abstract
We argue that the phase transition in the mean-field model is related to a particular change in the topology of its configuration space. The nature of this topological change can be discussed on the basis of elementary Morse theory using the potential energy per particle as a Morse function. The value of where such a topological change occurs equals the thermodynamic value of at the phase transition and the number of (Morse) critical points grows very fast with the number of particles . Furthermore, as in statistical mechanics, the way the thermodynamic limit is taken is crucial in topology.
- Received 30 October 1998
DOI:https://doi.org/10.1103/PhysRevLett.82.4160
©1999 American Physical Society