Observation of linear and nonlinear light trapping on topological dislocations

TL;DR

This paper experimentally demonstrates the first optical-frequency waveguiding at topological dislocations, revealing localized states and dislocation solitons that showcase the interplay of nonlinearity and topological defects in photonic lattices.

Contribution

It introduces the first observation of topological dislocation modes and dislocation solitons in optical systems, with precise control over their properties using femtosecond laser-writing.

Findings

Localized photonic eigenstates at dislocations with tunable shapes

Bifurcation of thresholdless dislocation solitons in high-power regimes

Control over mode localization and internal structure

Abstract

Topological dislocations in otherwise periodic lattices represent global structural defects that, nevertheless, typically leave the lattice periodicity intact far from the dislocation. Such dislocations arise in diverse physical systems ranging from crystalline solids, acoustic and photonic lattices and crystals to matter waves in optical lattices. Dislocations drastically affect the evolution of wave excitations in their vicinity, enabling novel mechanisms for trapping on topological defects and controlling the energy flow. Moreover, when combined with nonlinearity, such systems give rise to new types of self-sustained states of topological origin that have never been observed to date. Here we demonstrate experimentally, for the first time at optical frequencies, the waveguiding at various types of topological edge dislocations, resulting in the formation of localized photonic eigenstates with distinct and tunable shapes. Using femtosecond laser-writing techniques, we fabricated waveguide arrays with precisely tailored dislocation parameters, enabling full control over the degree of localization and internal structure of the associated modes. We further demonstrate both theoretically and experimentally that in the high-power regime, the families of thresholdless dislocation solitons bifurcate from such modes, which inherit shape diversity of their linear counterparts. Our results reveal a nontrivial interplay between nonlinearity and global lattice deformations and establish dislocation solitons as a new class of nonlinear topological states. They may stimulate the observation of new types of nonlinear states and interaction scenarios for excitations in nonlinear physical systems, where lattices with controllable global deformations can be created.