Abstract
We consider a generalization of the fixed and bounded trace ensembles introduced by Bronk and Rosenzweig up to an arbitrary polynomial potential. In the large- limit we prove that the two are equivalent and that their eigenvalue distribution coincides with that of the canonical ensemble with measure The mapping of the corresponding phase boundaries is illuminated in an explicit example. In the case of a Gaussian potential we are able to derive exact expressions for the one- and two-point correlator for finite n, having finite support.
- Received 5 October 1998
DOI:https://doi.org/10.1103/PhysRevE.59.1489
©1999 American Physical Society