TY - GEN
T1 - Ultrahigh-Q nanocavities fabricated by scanning probe microscope lithography on pre-patterned photonic crystal
AU - Yokoo, Atsushi
AU - Tanabe, Takasumi
AU - Kuramochi, Eiichi
AU - Notomi, Masaya
PY - 2011
Y1 - 2011
N2 - The attractiveness of a photonic crystal can be attributed to its unique optical characteristics. Specifically, the photonic crystal cavity provides strong light confinement, and enables the switching of light with very low threshold power. In a conventional process, to add this functionality, we have to modify its periodical structure during the CAD data processing step before electron beam lithography. This requirement limits the freedom of fabrication process. We can eliminate this limitation by taking advantage of the mode gap phenomena, with which we can furnish new cavity in the pre-patterned photonic crystal structure. The details of our cavity formation mechanism are described in reference 1). In Fig. 1(b), the pre-patterned structure is a line defect waveguide in a two-dimensional (2D) photonic crystal slab, and we assume that the refractive index is modulated in the yellow shaded region. A very small spatial index modulation (δn/n < 0.1%) changes the mode-gap edge frequency of the modified area to create barrier regions, while the unmodified area retains its original mode-gap edge frequency. As a result, an ultrahigh-Q cavity with a small volume can be created.
AB - The attractiveness of a photonic crystal can be attributed to its unique optical characteristics. Specifically, the photonic crystal cavity provides strong light confinement, and enables the switching of light with very low threshold power. In a conventional process, to add this functionality, we have to modify its periodical structure during the CAD data processing step before electron beam lithography. This requirement limits the freedom of fabrication process. We can eliminate this limitation by taking advantage of the mode gap phenomena, with which we can furnish new cavity in the pre-patterned photonic crystal structure. The details of our cavity formation mechanism are described in reference 1). In Fig. 1(b), the pre-patterned structure is a line defect waveguide in a two-dimensional (2D) photonic crystal slab, and we assume that the refractive index is modulated in the yellow shaded region. A very small spatial index modulation (δn/n < 0.1%) changes the mode-gap edge frequency of the modified area to create barrier regions, while the unmodified area retains its original mode-gap edge frequency. As a result, an ultrahigh-Q cavity with a small volume can be created.
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U2 - 10.1109/PHO.2011.6110558
DO - 10.1109/PHO.2011.6110558
M3 - Conference contribution
AN - SCOPUS:84856011351
SN - 9781424489404
T3 - IEEE Photonic Society 24th Annual Meeting, PHO 2011
SP - 324
EP - 325
BT - IEEE Photonic Society 24th Annual Meeting, PHO 2011
T2 - 24th Annual Meeting on IEEE Photonic Society, PHO 2011
Y2 - 9 October 2011 through 13 October 2011
ER -