Resonances in open quantum systems
arXiv:1608.08006 · doi:10.1103/PhysRevA.95.022117
Abstract
The Hamilton operator of an open quantum system is non-Hermitian. Its eigenvalues are, generally, complex and provide not only the energies but also the lifetimes of the states of the system. The states may couple via the common environment of scattering wavefunctions into which the system is embedded. This causes an {\it external mixing} (EM) of the states. Mathematically, EM is related to the existence of singular (the so-called exceptional) points (EPs). The eigenfunctions of a non-Hermitian operator are biorthogonal, in contrast to the orthogonal eigenfunctions of a Hermitian operator. A quantitative measure for the ratio between biorthogonality and orthogonality is the phase rigidity of the wavefunctions. At and near an EP, the phase rigidity takes its minimum value. The lifetimes of two nearby eigenstates of a quantum system bifurcate under the influence of an EP. At the parameter value of maximum width bifurcation, the phase rigidity approaches the value one, meaning that the two eigenfunctions become orthogonal. However, the eigenfunctions are externally mixed at this parameter value. The S-matrix and therewith the cross section do contain, in the one-channel case, almost no information on the EM of the states. The situation is completely different in the case with two (or more) channels where the resonance structure is strongly influenced by the EM of the states and interesting features of non-Hermitian quantum physics are revealed. We provide numerical results for two and three nearby eigenstates of a non-Hermitian Hamilton operator which are embedded in one common continuum and influenced by two adjoining EPs. The results are discussed. They are of interest for an experimental test of the non-Hermitian quantum physics as well as for applications.
Title of the paper is changed. The Introduction is broaden. The difference of the non-Hermitian formalism for the description of open quantum systems in our paper to the description of PT-symmetric systems is underlined. Paper published: Phys.Rev.A 95, 022117 (2017)
References in corpus (4)
- The physics of exceptional points
- Experimental Width Shift Distribution: A Test of Nonorthogonality for Local and Global Perturbations
- Phase rigidity and avoided level crossings in the complex energy plane
- Correlated behavior of conductance and phase rigidity in the transition from the weak-coupling to the strong-coupling regime
Cited by in corpus (4)
- Unified theory of resonances and bound states in the continuum in Hermitian tight-binding models
- Interference Effects in a Tunable Quantum Point Contact Integrated with an Electronic Cavity
- Bound states emerging from below the continuum in a solvable PT-symmetric discrete Schroedinger equation
- Time reversal of a discrete system coupled to a continuum based on non-Hermitian flip