Optical trimer: A theoretical physics approach to waveguide couplers

TL;DR

This paper uses group theory, specifically $SU(3)$ symmetry, to analyze and optimize waveguide couplers, providing a practical tutorial and exploring various configurations like equilateral and isosceles trimers for stable optical propagation.

Contribution

It introduces a symmetry-based, group-theory approach to design and analyze triangular waveguide couplers, linking their properties to mathematical structures like $SU(3)$ and cyclic groups.

Findings

Relation of equilateral trimer to Discrete Fourier Transform

Isosceles trimer's connection to the golden ratio and stability

Ability to derive coupled-mode equations for intensity and phase

Abstract

We study electromagnetic field propagation through an ideal, passive, triangular three-waveguide coupler using a symmetry based approach to take advantage of the underlying $SU(3)$ symmetry. The planar version of this platform has proven valuable in photonic circuit design providing optical sampling, filtering, modulating, multiplexing, and switching. We show that a group-theory approach can readily provide a starting point for design optimization of the triangular version. Our analysis is presented as a practical tutorial on the use of group theory to study photonic lattices for those not familiar with abstract algebra methods. In particular, we study the equilateral trimer to show the relation of pearl-necklace arrays with the Discrete Fourier Transform due to their cyclic group symmetry, and the isosceles trimer to show its relation with the golden ratio and its ability to provide stable output at a single waveguide. We also study the propagation dependent case of an equilateral trimer that linearly increases or decreases its effective coupling with the propagation distance. For the sake of completeness, we go beyond the standard optical-quantum analogy to show that it is possible to derive coupled-mode equations for intensity and phase, and that it is also possible to calculate envelopes for the propagation of all possible inputs belonging to an energy class, as well as individual input field amplitudes, without the need of point-to-point propagation.