Magnetic doping-induced second-order and first-order topological phase transition inthe photonic alloy

TL;DR

This paper demonstrates a controllable topological phase transition in a 2D photonic alloy by magnetic doping, switching between second-order corner states and first-order chiral edge states, with potential for tunable topological photonic devices.

Contribution

It introduces a magnetic doping method to induce and control topological phase transitions in a disordered photonic system, extending topological physics understanding.

Findings

Zero doping shows higher-order corner states with trivial Chern number and bulk polarization 1/3.

Increasing doping merges corner states with bulk, closing the gap.

Further doping reopens the gap, resulting in a first-order phase with chiral edge states and Chern number -1.

Abstract

The bulk-edge correspondence principle, a cornerstone of topological physics, ensures that first-order topological systems host robust chiral edge states in two dimension. This was later extended to higher-order phases, where second-order topological insulators exhibit localized, topologically protected corner states. While the transition between these distinct phases has been demonstrated in periodic systems, its existence in disordered platforms remains an open question. Here, we demonstrate a controllable topological phase transition between a second-order topological phase and a first-order topological phase in a two-dimensional photonic alloy. By tuning the magnetic doping concentration - implemented by attaching permanent magnets randomly to nonmagnetized yttrium iron garnet rods in an alternately magnetized honeycomb lattice with C3 rotational symmetry - we flexibly control the system's topology. At zero doping, we observe higher-order corner states, confirmed by a trivial Chern number and non-zero bulk polarizations of 1/3. As doping concentration increases, these corner states progressively merge with the bulk states, culminating in the closure of the bulk transmission gap. After the bulk transmission gap reopens with further increased doping, the system transitions to a first-order topological phase, characterized by a nontrivial Chern number of -1 and the emergence of a chiral edge state. This transition is reversible, providing a highly tunable and experimentally simple platform for flexibly switching between localized corner states and delocalized chiral edge states within a single photonic system.