Consistent quantum treatments of non-convex kinetic energies

TL;DR

This paper investigates how to consistently relate quantum Hamiltonians and classical Lagrangians for systems with nonconvex kinetic energies, revealing phase transitions and resolving apparent inconsistencies.

Contribution

It introduces a framework showing that nonconvex kinetic energies can be valid under certain conditions, especially with environmental coupling, and offers methods to handle such anomalous theories.

Findings

Identification of a dissipative phase transition between Hamiltonian and Lagrangian regimes

Demonstration of exceptional points in imaginary time

Provision of computational methods for nonconvex kinetic energies

Abstract

The task of finding a consistent relationship between a quantum Hamiltonian and a classical Lagrangian is of utmost importance for basic, but ubiquitous techniques like canonical quantization and path integrals. Nonconvex kinetic energies (which appear, e.g., in nonlinear capacitors or classical time crystals) pose a fundamental problem: the Legendre transformation is ill-defined, and the more general Legendre-Fenchel transformation removes nonconvexity essentially by definition. Arguing that such anomalous theories follow from suitable low-energy approximations of well-defined, harmonic theories, we show that seemingly inconsistent Hamiltonian and Lagrangian descriptions can both be valid, depending on the coupling strength to a dissipative environment. There occurs a dissipative phase transition from a nonconvex Hamiltonian to a convex Lagrangian regime, involving exceptional points in imaginary time. Our approach thus resolves apparent inconsistencies and provides computationally efficient methods to treat anomalous, nonconvex kinetic energies.