Coupled mode theory

Coupled mode theory first arose in the 1950s in the works of Miller on microwave transmission lines,[1] Pierce on electron beams,[2] and Gould on backward wave oscillators.[3] This put in place the mathematical foundations for the modern formulation expressed by H. A. Haus et al. for optical waveguides.[4][5]

In the late 1990s and early 2000s, the field of nanophotonics has revitalized interest in coupled mode theory. Coupled mode theory has been used to account for the Fano resonances in photonic crystal slabs[6] and has also been modified to account for optical resonators with non-orthogonal modes.[7]

The oscillatory systems to which coupled mode theory applies are described by second order partial differential equations (e.g. a mass on a spring, an RLC circuit). CMT allows the second order differential equation to be expressed as one or more uncoupled first order differential equations. The following assumptions are generally made with CMT:

• Linearity
• Time-reversal symmetry
• Time-invariance
• Weak mode coupling (small perturbation of uncoupled modes)
• Energy conservation

The formulation of the coupled mode theory is based on the development of the solution to an electromagnetic problem into modes. Most of the time it is eigenmodes which are taken in order to form a complete base. The choice of the base and the adoption of certain hypothesis like parabolic approximation differs from formulation to formulation. The classification proposed by [8] of the different formulation is as follows:

1. The choice of starting differential equation. some of the coupled mode theories are derived directly from the Maxwell differential equations [9][10] (here) although others use simplifications in order to obtain a Helmholtz equation.
2. The choice of principle to derive the equations of the CMT. Either the reciprocity theorem [9][10] or the variational principle have been used.
3. The choice of orthogonality product used to establish the eigenmode base. Some references use the unconjugated form [9] and others the complex-conjugated form.[10]
4. Finally, the choice of the form of the equation, either vectorial [9][10] or scalar.

When n modes of an electromagnetic wave propagate through a media in the direction z without loss the power transported by each mode is described by a modal power Pm. At a given frequency ω.

${\displaystyle P^{\omega }(z)=\sum _{m}^{n}P_{m}^{\omega }(z)={\frac {1}{4}}\sum _{m}^{n}N_{m}^{\omega }\left|a_{m}^{\omega }(z)\right|^{2}\,\!}$

where N_m is the norm of the mth mode and a_m is the modal amplitude.

• Eigenmode expansion

• WMM mode solver manual on couple mode theory
• Coupled-Mode Theory and Devices (see and listen to Lectures 5 and 6)