Fractal and chaotic solutions of the discrete nonlinear Schr\"odinger equation in classical and quantum systems

TL;DR

This paper explores complex, chaotic, and fractal solutions of the discrete nonlinear Schrödinger equation in quantum and classical lattice systems, revealing irregular structures in wave functions and energy spectra.

Contribution

It provides a method for obtaining numerically exact solutions of the DNSE and demonstrates the emergence of chaotic and incommensurate states in various physical models.

Findings

Wave functions can exhibit incommensurate and irregular structures.

Exact energy spectra are obtained in the strong coupling limit.

Wave functions at moderate coupling agree with strong coupling results.

Abstract

We discuss stationary solutions of the discrete nonlinear Schr\"odinger equation (DNSE) with a potential of the $\phi^{4}$ type which is generically applicable to several quantum spin, electron and classical lattice systems. We show that there may arise chaotic spatial structures in the form of incommensurate or irregular quantum states. As a first (typical) example we consider a single electron which is strongly coupled with phonons on a $1D$ chain of atoms --- the (Rashba)--Holstein polaron model. In the adiabatic approximation this system is conventionally described by the DNSE. Another relevant example is that of superconducting states in layered superconductors described by the same DNSE. Amongst many other applications the typical example for a classical lattice is a system of coupled nonlinear oscillators. We present the exact energy spectrum of this model in the strong coupling limit and the corresponding wave function. Using this as a starting point we go on to calculate the wave function for moderate coupling and find that the energy eigenvalue of these structures of the wave function is in exquisite agreement with the exact strong coupling result. This procedure allows us to obtain (numerically) exact solutions of the DNSE directly. When applied to our typical example we find that the wave function of an electron on a deformable lattice (and other quantum or classical discrete systems) may exhibit incommensurate and irregular structures. These states are analogous to the periodic, quasiperiodic and chaotic structures found in classical chaotic dynamics.