Breit-Wigner to Gaussian transition in strength functions
Nuclear Theory
2007-05-23 v1 Chaotic Dynamics
Abstract
Employing hamiltonians defined by two-body embedded Gaussian orthogonal ensemble of random matrices(EGOE(2)) plus a mean-field producing one-body part, strength functions (for states defined by the one-body part) are constructed for various values of the strength of the chaos generating two-body part. Numerical calculations for six and seven fermion systems clearly demonstrate Breit-Wigner to Gaussian transition, in the chaotic domain, in strength functions as found earlier in nuclear shell model and Lipkin-Meshkov-Glick model calculations.
Cite
@article{arxiv.nucl-th/0006079,
title = {Breit-Wigner to Gaussian transition in strength functions},
author = {V. K. B. Kota and R. Sahu},
journal= {arXiv preprint arXiv:nucl-th/0006079},
year = {2007}
}
Comments
7 pages, 2 figures, submitted to Phys. Rev. C