Abstract
An approximate solution at the critical point of the spherical to axially deformed shape phase transition in nuclei is presented. The eigenvalues of the Hamiltonian are expressed in terms of zeros of Bessel functions of irrational order.
- Received 12 December 2000
DOI:https://doi.org/10.1103/PhysRevLett.87.052502
©2001 American Physical Society
