Abstract

In comparison with conventional lasers, topological lasers are more robust and can be immune to disorder or defects if lasing occurs in topologically protected states. Previously reported topological lasers were almost exclusively based on the first-order photonic topological insulators. Here, we show that lasing can be achieved in the zero-dimensional corner state in a second-order photonic topological insulator, which is based on the Kagome waveguide array with a rhombic configuration. If gain is present in the corner of the structure, where the topological corner state resides, stable lasing in this state is achieved, with the lowest possible threshold, in the presence of uniform losses and two-photon absorption. When gain acts in other corners of the structure, lasing may occur in edge or bulk states, but it requires substantially larger thresholds, and transition to stable lasing occurs over much larger propagation distances, sometimes due to instabilities, which are absent for lasing in corner states. We find that increasing two-photon absorption generally plays strong stabilizing action for nonlinear lasing states. The transition to stable lasing stimulated by noisy inputs is illustrated. Our work demonstrates the realistic setting for corner state lasers based on higher-order topological insulators realized with waveguide arrays.

Highlights

  • A d-dimensional topological insulator supports bulk states and (d − l)D topological edge states

  • We show that lasing can be achieved in the zero-dimensional corner state in a second-order photonic topological insulator, which is based on the Kagome waveguide array with a rhombic configuration

  • If gain is present in the corner of the structure, where the topological corner state resides, stable lasing in this state is achieved, with the lowest possible threshold, in the presence of uniform losses and two-photon absorption

Read more

Summary

INTRODUCTION

A d-dimensional (dD) topological insulator supports (dD) bulk states and (d − l)D topological edge states. Scitation.org/journal/app the corresponding governing equations, determines the amplitudes of lasing modes These effects were employed for the realization of so-called topological lasers[35–41] representing a novel extension of the concept of topological insulators. We provide the illustration of topological corner lasers on a new platform—shallow waveguide arrays (as opposed to previous works on microrings or photonic crystal cavities with a 2D SSH configuration)—the idea that can be extended to polaritonic systems based on micropillar arrays, where nonlinear interactions of polaritons are repulsive[36,51,52] (in our case, nonlinearity is attractive). The detailed analysis of stability of lasing modes is provided for different values of linear gain and two-photon absorption coefficients It is illustrated how lasing in corner states builds up from random noisy inputs. In corner lasers, the appearance of topological modes is guaranteed by simple deformation of the structure, allowing miniaturization and increasing performance in the nonlinear regime

Band structure and linear modes of the conservative system
Linear modes of the dissipative system
Families of nonlinear lasing modes
Noise-stimulated lasing
Discussion
CONCLUSIONS
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call