Nuclear fission with mean-field instantons

TL;DR

This paper introduces a novel instanton-based approach to describe nuclear spontaneous fission and quantum tunneling, comparing it with existing methods and highlighting its advantages in estimating decay rates.

Contribution

It develops a mean-field instanton framework for nuclear fission, establishing a minimum principle for the action functional and connecting it with traditional methods like GCM and ATDHF.

Findings

Instanton action fulfills a minimum principle with constraints.

GCM inertia overestimates decay rates compared to instantons.

Inclusion of pairing leads to a variational formulation in TDHFB theory.

Abstract

We present a description of nuclear spontaneous fission, and generally of quantum tunneling, in terms of instantons - periodic imaginary-time solutions to time-dependent mean-field equations - that allows for a comparison with more familiar and used generator coordinate (GCM) and adiabatic time-dependent Hartree-Fock (ATDHF) methods. It is shown that the action functional whose value for the instanton is the quasiclassical estimate of the decay exponent fulfils the minimum principle when additional constraints are imposed on trial fission paths. In analogy with mechanics, these are conditions of energy conservation and the velocity-momentum relations. In the adiabatic limit the instanton method reduces to the time-odd ATDHF equation, with collective mass including the time-odd Thouless-Valatin term, while the GCM mass completely ignores velocity-momentum relations. This implies that GCM inertia generally overestimates instanton-related decay rate. The very existence of the minimum principle offers a hope for a variational search for instantons. After the inclusion of pairing, the instanton equations and the variational principle can be expressed in terms of the imaginary-time-dependent Hartree-Fock- Bogolyubov (TDHFB) theory. The adiabatic limit of this theory reproduces ATDHFB inertia.