Topological materials
Can light's frequency act as an extra dimension for topology?
Open access · cc by · source: Europe PMC
Simulations show that pairs of modulated ring resonators can use light's frequency as an extra dimension to build a higher-order topological insulator whose corner states resist disorder.
Study at a glance
- Design
- Computational / modelling — Theory plus numerical coupled-mode simulations (rotating-wave approximation and full time-dependent dynamics) of arrays of electro-optically modulated ring resonators.
- N
- No sample; simulations of a finite lattice of ten frequency sites by six rings.
- Population
- Simulated photonic ring-resonator lattices ("photonic molecules") with a synthetic frequency axis
- Outcome
- Corner, edge and bulk mode spectra and field distributions; robustness to disorder; phase transition as modulation phase changes
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Key findings
In the topological regime the simulated array showed a transmission peak pinned at zero detuning with light strongly localised at the corner, while edge and bulk modes appeared at gapped detunings; in the trivial regime no mid-gap peak existed. Changing the relative modulation phase from pi to zero drove a transition to a 2D SSH phase whose bulk gap closes. With disorder, corner modes stayed well separated and localised in the quadrupole phase but leaked into the bulk in the zero-flux phase. Corner localisation survived moderate modulation beyond the rotating-wave approximation but degraded under ultrastrong modulation.
Methodology
The authors designed a chain of paired ring resonators whose modulation couples neighbouring frequency modes, turning frequency into a synthetic lattice axis alongside one real spatial axis. Choosing the modulation phases to give a flux of pi per plaquette reproduces the Benalcazar-Bernevig-Hughes quadrupole model. They simulated driving the array through external waveguides, compared approximate and full dynamical solutions, added coupling disorder, and extended the recipe to octupole and 16-pole (four-dimensional) lattices.
Limitations
Everything is simulated; no device was built, so fabrication imperfections, loss and the practicality of modulating near the free spectral range are untested. The frequency lattice must be artificially truncated to have corners, which the authors only suggest ways to achieve. The octupole and hexadecapole designs are constructed conceptually rather than analysed in depth, and the model neglects dispersion in the ring-to-ring coupling.
How this study connects
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