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WAVES AND VIBRATIONS IN INHOMOGENEOUS STRUCTURES ...

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4.4 Ridge waveguides 39<br />

w<br />

ε =1<br />

?<br />

ε<br />

a) b) c)<br />

Figure 4.7 a) Design problem for a 2D model of a photonic ridge waveguide splitter.<br />

The objective is to distribute 50% of the input energy into the top and bottom output<br />

ports and thus avoid reflection and radiation at the T-junction, b) optimized design for<br />

E-polarized waves, c) optimized design for H-polarized waves. Black: dielectric material,<br />

light gray: air. From paper [17].<br />

4.4 Ridge waveguides<br />

The examples of optimized waveguide components are all based on waveguides<br />

carved out in photonic crystal structures. This provides a basis for confinement<br />

of the light which is very useful for waveguiding purposes. However, another type<br />

of waveguides, denoted strip or ridge waveguides, are applicable to photonic circuits<br />

as well. These consist of dielectric strips with a rectangular cross section placed on<br />

a substrate and surrounded by air. Such strips may provide perfect waveguiding for<br />

straight guides. However, the problems at bends and junctions are even more severe<br />

than for photonic crystal waveguides in that the waves are no longer confined to the<br />

guide and thus additional in-plane scattering losses may be induced.<br />

Nevertheless, the same design procedure can be applied as for the photonic crystal<br />

waveguide components. Fig. 4.7a shows an optimization problem for the design<br />

of a T-junction in a 2D model of a ridge waveguide. The optimized junctions in<br />

Fig. 4.7b,c correspond to the case of E- and H-polarized waves, respectively. In both<br />

cases the optimization is performed for waves with a wavelength close to 1550nm<br />

which is relevant for telecommunication purposes 4 .<br />

For both optimized junctions the obtained efficiency is close to 100% near the<br />

wavelength 1550nm, yet, the required junction area is larger (relative to the strip<br />

width w) for the case of the E-polarized waves (Fig. 4.7b). This is due to the<br />

wavelength/strip width ratio being larger for this polarization. If a smaller design<br />

domain is used, the efficiency is reduced accordingly. Fig. 4.7c illustrates also that<br />

4 It should be noted that the two different polarizations correspond to two different values of<br />

the strip width w and dielectric constant ε.

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