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Two-Dimensional Photonic-BandGap Structures Operating at Near-Infrared Wavelengths

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Abstract

Photonic crystals are artificial structures having a periodic dielectric structure designed to influence the behaviour of photons in much the same way that the crystal structure of a semiconductor affects the properties of electrons *RF 1*. In particular, photonic crystals forbid propagation of photons having a certain range of energies (known as a photonic bandgap), a property that could be incorporated in the design of novel optoelectronic devices [2]. Following the demonstration of a material with a full photonic bandgap at microwave frequencies [3], there has been considerable progress in the fabrication of three-dimensional photonic crystals with operational wavelengths as short as 1.5 micrometer [4], although the optical properties of such structures are still far from ideal [5]. Here we show that, by restricting the geometry of the photonic crystal to two dimensions (in a waveguide configuration), structures with polarization-sensitive photonic bandgaps at still lower wavelengths (in the range 800-900 nm) can be readily fabricated. Our approach should permit the straightforward integration of photonic-bandgap structures with other optical and optoelectronic devices.
... [42][43][44][45][46] Periodic structures further provide precise control over wave propagation and dispersion. For instance, photonic crystals manipulate electromagnetic waves to create peculiar phenomena such as photonic bandgaps, [47][48][49] resonant field enhancement and localization, [50][51][52] and slow-light effects, [53][54][55] which have been leveraged to achieve high sensitivities in PhC-based sensors. [56][57][58] Similarly, phononic [59] and magnonic [60] crystals enable the control of acoustic and spin waves, respectively. ...
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... We start from Maxwell's equations in an anisotropic medium, incorporating correction terms representing nonlinear polarization and higher-order electromagnetic effects [10,19] : ...
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