PT-Symmetric Nonlinear Metamaterials and Zero-Dimensional Systems

TL;DR

This paper explores ${ m PT}$-symmetric nonlinear magnetic metamaterials, revealing phase transitions, localized nonlinear modes called breathers, and a zero-dimensional ${ m PT}$ system with a transition from oscillatory to diverging behavior.

Contribution

It introduces a novel ${ m PT}$-symmetric metamaterial model with nonlinear localized modes and a simple harmonic oscillator model demonstrating ${ m PT}$ symmetry in zero dimensions.

Findings

Transition from exact to broken ${ m PT}$ phase in linear spectra.

Existence of long-lived nonlinear breathers supported by gain.

A zero-dimensional ${ m PT}$ system exhibits a transition from oscillatory to diverging motion.

Abstract

A one dimensional, parity-time (${\cal PT}$)-symmetric magnetic metamaterial comprising split-ring resonators having both gain and loss is investigated. In the linear regime, the transition from the exact to the broken ${\cal PT}$-phase is determined through the calculation of the eigenfrequency spectrum for two different configurations; the one with equidistant split-rings and the other with the split-rings forming a binary pattern (${\cal PT}$ dimer chain). The latter system features a two-band, gapped spectrum with its shape determined by the gain/loss coefficient as well as the inter-element coupling. In the presense of nonlinearity, the ${\cal PT}$ dimer chain with balanced gain and loss supports nonlinear localized modes in the form of novel discrete breathers below the lower branch of the linear spectrum. These breathers, that can be excited from a weak applied magnetic field by frequency chirping, can be subsequently driven solely by the gain for very long times. The effect of a small imbalance between gain and loss is also considered. Fundamendal gain-driven breathers occupy both sites of a dimer, while their energy is almost equally partitioned between the two split-rings, the one with gain and the other with loss. We also introduce a model equation for the investigation of classical ${\cal PT}$ symmetry in zero dimensions, realized by a simple harmonic oscillator with matched time-dependent gain and loss that exhibits a transition from oscillatory to diverging motion. This behaviour is similar to a transition from the exact to the broken ${\cal PT}$ phase in higher-dimensional ${\cal PT}-$ symmetric systems. A stability condition relating the parameters of the problem is obtained in the case of piecewise constant gain/loss function that allows for the construction of a phase diagram with alternating stable and unstable regions.