Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group

Ultra-compact 32-channel drop filter with 100 GHz spacing

Open Access Open Access

Abstract

We demonstrated 32-channel drop filters with 100 GHz spacing consisting of arrayed nanocavities and a waveguide in a photonic crystal silicon slab. Changing the lattice constant of the nanocavities on the subnanometer scale successfully controlled the drop wavelengths at 100 GHz spacing in the wavelength range between 1510 and 1550 nm. The device size was as small as 15 μm × 270 μm, and the variation in drop wavelengths was less than 0.3 nm in terms of standard deviation. We also present a movie showing the operation of the drop filter, demonstrating that the arrayed nanocavities have the potential for developing ultracompact 100 GHz spaced filters in a dense wavelength division multiplexing system.

© 2014 Optical Society of America

Full Article  |  PDF Article
More Like This
Ultrahigh-Q photonic crystal nanocavities fabricated by CMOS process technologies

Kohei Ashida, Makoto Okano, Minoru Ohtsuka, Miyoshi Seki, Nobuyuki Yokoyama, Keiji Koshino, Masahiko Mori, Takashi Asano, Susumu Noda, and Yasushi Takahashi
Opt. Express 25(15) 18165-18174 (2017)

Towards 100 channel dense wavelength division multiplexing with 100GHz spacing on silicon

D. T. H. Tan, A. Grieco, and Y. Fainman
Opt. Express 22(9) 10408-10415 (2014)

Highly efficient multi-channel drop filter in a two-dimensional hetero photonic crystal

Hitomichi Takano, Bong-Shik Song, Takashi Asano, and Susumu Noda
Opt. Express 14(8) 3491-3496 (2006)

Supplementary Material (2)

Media 1: AVI (1096 KB)     
Media 2: AVI (2225 KB)     

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (5)

Fig. 1
Fig. 1 (Upper) Confocal laser scanning microscope image of a 32-channel drop filter which consists of 32 photonic crystal units, PC1–PC32. (Lower) SEM view of a 0.2a shifted L3 nanocavity for the unit PCn. The lattice constant an in the x-direction was {410−0.375 × (n−1)} nm. We fabricated three samples with air holes of different radii.
Fig. 2
Fig. 2 Measurement setup used to investigate the drop wavelengths of arrayed nanocavities. Pol: polarizer. OL: objective lens. BS: beam splitter. M: mirror on a flip mount stage. PD: InGaAs photodiode. NIR camera: near-infrared InGaAs camera.
Fig. 3
Fig. 3 (a) Wavelength of dropped light versus the lattice constant in the x direction for 32 arrayed nanocavities. Open circles represent experimental data, and red lines indicate linear fits. The inset is the calculated resonant wavelength of the nanocavities. (b) Histogram of wavelength deviations for the three samples.
Fig. 4
Fig. 4 Near-infrared camera shots of the 32-channel drop filter with r = 110 nm when the wavelength of the transmitted laser was scanned from 1525 to 1545 nm at a speed of 2 nm per second (Media 1). A movie showing the operation of the drop filter consisting of 0.15a shifted L3 cavities is presented in Media 2. Movies were obtained with exposure time of 10 millisecond, 25 frames per second, and camera resolution of 320 × 256 pixels.
Fig. 5
Fig. 5 (a) Normalized drop spectra for 32 nanocavities in the sample with r = 110 nm. (b) Histogram of the Qexp values for 32 channels. (c) Histogram of the drop efficiencies.

Equations (2)

Equations on this page are rendered with MathJax. Learn more.

1 Q exp = 1 Q des + 1 Q in + 1 Q imp .
η drop = ( Q in / Q des ) ( 1+ Q in / Q des ) 2 .
Select as filters


Select Topics Cancel
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.