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Frontiers of Optoelectronics

ISSN 2095-2759

ISSN 2095-2767(Online)

CN 10-1029/TN

Postal Subscription Code 80-976

Front Optoelec    2012, Vol. 5 Issue (1) : 78-81    https://doi.org/10.1007/s12200-012-0199-4
RESEARCH ARTICLE
Binary blazed grating-based polarization-independent filter on silicon on insulator
Danhua WU, Xin SUI, Junbo YANG, Zhiping ZHOU()
The State Key Laboratory of Advanced Optical Communication Systems and Networks, Peking University, Beijing 100871, China
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Abstract

In this paper, a binary blazed grating-based polarization independent filter on silicon on insulator (SOI) under full conical incidence is presented. The properties of the grating filter are investigated by rigorous coupled-wave analysis. It’s shown that the filter demonstrates high reflectivity (R>99%) at its resonant wavelength, which stays the same under three different polarization states. It indicates that this grating filter is polarization-independent. The final data shows its polarization-dependent loss (PDL) is only 0.04 dB and the full width at half maximums (FWHMs) of the transverse electric (TE-) and transverse magnetic (TM-) polarized light are 0.24 and 0.46 nm, respectively.

Keywords narrow filter      binary blazed grating      full conical incidence      polarization-independent     
Corresponding Author(s): ZHOU Zhiping,Email:zjzhou@pku.edu.cn   
Issue Date: 05 March 2012
 Cite this article:   
Junbo YANG,Zhiping ZHOU,Danhua WU, et al. Binary blazed grating-based polarization-independent filter on silicon on insulator[J]. Front Optoelec, 2012, 5(1): 78-81.
 URL:  
https://academic.hep.com.cn/foe/EN/10.1007/s12200-012-0199-4
https://academic.hep.com.cn/foe/EN/Y2012/V5/I1/78
Fig.1  Coordinate system for binary blazed grating in conical mounting
Fig.2  Full conical incidence for resonant excitation of two identical guided-modes
Fig.3  Scheme of SOI-based polarization-independent filter using binary blazed grating
f1f2f3θ/(o)α/(o)T/nmtg/nmtw/nm
0.4320.7350.874459070070250
Tab.1  Optimized parameters of grating filter
Fig.4  PDL curves under different grating periods and depths. (a) As a function of grating period. All other parameters are the same as those in Table 1; (b) as a function of grating depth. All other parameters are the same as those in Table 1
Fig.5  Spectral reflectivity of the filter based on binary blazed grating
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