Field localisation and spin-momentum locking in zero-dimensional dissipative topological photonic interface state

TL;DR

This paper demonstrates how zero-dimensional topological interface states in dissipative photonic crystals exhibit strong field localization and spin-momentum locking, with potential applications in controlling electromagnetic fields.

Contribution

It introduces a novel 0D interface state arising from 1D dissipative topological photonic crystals, highlighting the role of complex Dirac mass parameters in field localization and spin-momentum locking.

Findings

Strong field localization at the interface

Observation of spin-momentum locking

Verification through simulations and spectroscopy

Abstract

Topological photonic systems support edge states that are robust against disorder and perturbation. Depending on the symmetry and dimensionality of the bulk systems, different edge states emulating soliton, quantum integer and quantum spin Hall effects have been realized. A major concern in photonics is how one can shape the strength and polarisation of electromagnetic fields to suit different applications. Here, we show zero-dimensional (0D) interface state arising from one-dimensional (1D) dissipative topological photonic crystals exhibit strong field localisation and spin-momentum locking thanks to its complex classical analogue Dirac mass parameter. By using spatiotemporal coupled mode theory to formulate 1D photonic crystals and their corresponding Jackiw Rebbi-like (JR) interface state, we find the interaction between two energy bands at high symmetry points plays a major role in defining not only the topological triviality of the crystals but also its complex Dirac mass parameter. More importantly, when two topological trivial and nontrivial bulk systems are brought together to form a JR state, while the real part of the Dirac mass parameter governs the spectral and spatial field localisations of the interface state, the imaginary part gives rise to a net flow of energy towards the interface and a transverse spin angular momentum, resulting in a strong spin-momentum locking. We verify our theory by 1D plasmonic crystals using finite-difference time-domain simulations as well as far-field angle-resolved spectroscopy and imaging.