Width bifurcation and dynamical phase transitions in open quantum systems

TL;DR

This paper investigates how open quantum systems exhibit width bifurcation and phase transitions near exceptional points, revealing how different coupling components influence system stability and resonance behavior.

Contribution

It demonstrates the distinct effects of Re(ω) and Im(ω) on eigenvalue crossing and width bifurcation, highlighting the physical implications of these phenomena in open quantum systems.

Findings

Re(ω) causes eigenvalue avoided crossing near exceptional points.

Im(ω) leads to width bifurcation and system splitting.

Long-lived states have increased stability, short-lived states appear as background.

Abstract

The states of an open quantum system are coupled via the environment of scattering wavefunctions. The complex coupling coefficients $\omega$ between system and environment arise from the principal value integral and the residuum. At high level density where the resonance states overlap, the dynamics of the system is determined by exceptional points. At these points, the eigenvalues of two states are equal and the corresponding eigenfunctions are linearly dependent. It is shown in the present paper that Im$(\omega)$ and Re$(\omega)$ influence the system properties differently in the surrounding of exceptional points. Controlling the system by a parameter, the eigenvalues avoid crossing in energy near an exceptional point under the influence of Re$(\omega)$ in a similar manner as it is well known from discrete states. Im$(\omega)$ however leads to width bifurcation and finally (when the system is coupled to one channel, i.e. to a common continuum of scattering wavefunctions), to a splitting of the system into two parts with different characteristic time scales. Physically, the system is stabilized by this splitting since the lifetimes of most ($N-1$) states are longer than before while that of only one state is shorter. In the cross section the short-lived state appears as a background term in high-resolution experiments. The wavefunctions of the long-lived states are mixed in those of the original ones in a comparably large parameter range. Numerical results for the eigenvalues and eigenfunctions are shown for $N=2, ~4$ and 10 states coupled mostly to 1 channel.