Abstract
Consider a system rendered unstable by both quantum tunneling and thermodynamic fluctuation. The tunneling rate , at temperature , is related to the free energy by . However, the classical escape rate is , being the negative eigenvalue at the saddle point. A general theory of metastability is constructed in which these formulas are true for temperatures, respectively, below and above with a narrow transition region of .
- Received 22 September 1980
DOI:https://doi.org/10.1103/PhysRevLett.46.388
©1981 American Physical Society