Optical ring resonators are commonly discussed on the basis of a frequency-domain model, that divides a resonator into coupler elements, ring cavity segments, and the straight port waveguides. We look at the assumptions underlying this model and at its implications, including remarks on reciprocity/symmetry arguments, the general power transfer characteristics, the resonance condition, the spectral distance and width of the resonances, the quantities that describe the resonator performance, and a few remarks about tuning. A survey of bend mode properties and a coupler description in terms of coupled mode theory fills the abstract notions of the model. As an example for devices that rely on a standing wave principle, in contrast to the traveling waves found in the microrings, we consider in less detail microresonators with square or rectangular cavity shapes. Also here a frequency domain coupled mode theory can be applied that opens up simple possibilities to characterize resonant configurations.
Abstract resonator modelThe "standard" model covers the propagation of light at fixed angular frequency ω = kc, usually specified by the vacuum wavelength λ , vacuum wavenumber k = 2π/λ , and vacuum speed of light c. All optical fields vary in time according to ∼ exp(iωt). The list of underlying assumptions and approximations includes the following items:• Single polarization operation is considered, none of the waveguide segments and coupler elements couples waves of different polarization; all waveguides are unimodal per polarization orientation.