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Two-dimensional photonic crystals in macroporous silicon: from mid-infrared (10 /spl mu/m) to telecommunication wavelengths (1.3-1.5 /spl mu/m)

We present a detailed study of two-dimensional (2D) photonic crystals based on macroporous silicon technology, showing a broad range of wavelengths accessible for applications with this material. In this work, we have reached 1.55 /spl mu/m, this certainly represents a decisive issue for this techno...

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Bibliographic Details
Published in:Journal of lightwave technology 1999-11, Vol.17 (11), p.1989-1995
Main Authors: Rowson, S., Chelnokov, A., Lourtioz, J.-M.
Format: Article
Language:English
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Summary:We present a detailed study of two-dimensional (2D) photonic crystals based on macroporous silicon technology, showing a broad range of wavelengths accessible for applications with this material. In this work, we have reached 1.55 /spl mu/m, this certainly represents a decisive issue for this technology. First, the reflection performances of a hexagonal and a triangular lattice of air holes are compared. The triangular lattice reduces technological requirements because the complete photonic bandgap (PBG) results from the overlap of broader forbidden bands of lower order. Second, a combined experimental and theoretical study is presented of the reflection properties of a 2D photonic crystal in a three-dimensional (3D) optical environment. This reveals the critical parameters that can degrade the performances of such 2-D structures. Reflection coefficients up to 98% are obtained with optical quality interfaces. Finally, a complete PBG centered at 1.55 /spl mu/m is demonstrated with a submicrometer period triangular lattice defined by holographic lithography. The influence of the air filling factor on the band position and the interface quality is analyzed by reflection measurements. The overall results show the high flexibility of the macroporous silicon technology and its applicability to integrated optics at telecommunication wavelengths.
ISSN:0733-8724
1558-2213
DOI:10.1109/50.802985