• Photonics Research
  • Vol. 5, Issue 3, 212 (2017)
Wentao Qiu1, Huihui Lu1、3, Fadi Issam Baida2、*, and Maria-Pilar Bernal2
Author Affiliations
  • 1Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Department of Optoelectronic Engineering, Jinan University, Guangzhou, China
  • 2Département d’Optique P.M. Duffieux, Institut FEMTO-ST, UMR 6174 CNRS Université Bourgogne Franche-Comté, 15B Avenue des Montboucons, 25030 Besançon Cedex, France
  • 3e-mail: thuihuilu@jnu.edu.cn
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    DOI: 10.1364/PRJ.5.000212 Cite this Article Set citation alerts
    Wentao Qiu, Huihui Lu, Fadi Issam Baida, Maria-Pilar Bernal. Ultra-compact on-chip slot Bragg grating structure for small electric field detection[J]. Photonics Research, 2017, 5(3): 212 Copy Citation Text show less
    (a) Sketch of 2D SWG considered in the 2D-FDTD simulations. (b) Sketch of 2D slot Bragg grating structure considered in the 2D-FDTD simulations. Period of grating a and width of air groove Wair is denoted in the figure. (c) Incident E-field profile in the 2D-FDTD slot Bragg grating simulations. The LN slot, silicon rails, and air ambient medium are denoted, respectively, in the figure. (d) Normalized transmission of 2D slot Bragg grating structure with parameters of a=340 nm, Wair=200 nm, and the number of air grooves N=10.
    Fig. 1. (a) Sketch of 2D SWG considered in the 2D-FDTD simulations. (b) Sketch of 2D slot Bragg grating structure considered in the 2D-FDTD simulations. Period of grating a and width of air groove Wair is denoted in the figure. (c) Incident E-field profile in the 2D-FDTD slot Bragg grating simulations. The LN slot, silicon rails, and air ambient medium are denoted, respectively, in the figure. (d) Normalized transmission of 2D slot Bragg grating structure with parameters of a=340  nm, Wair=200  nm, and the number of air grooves N=10.
    (a) Sketch of 2D slot Bragg gating structure with a defect size of Wd in the 2D-FDTD simulations. The period of grating a and the width of air groove Wair is denoted in the figure. (b) Normalized transmission of 2D slot Bragg grating structure with a symmetric F-P cavity with the parameters of a=370 nm, Wair=260 nm, Wd=290 nm, and number of air grooves on each side of defect N=5.
    Fig. 2. (a) Sketch of 2D slot Bragg gating structure with a defect size of Wd in the 2D-FDTD simulations. The period of grating a and the width of air groove Wair is denoted in the figure. (b) Normalized transmission of 2D slot Bragg grating structure with a symmetric F-P cavity with the parameters of a=370  nm, Wair=260  nm, Wd=290  nm, and number of air grooves on each side of defect N=5.
    E-field amplitude distribution of Ez component along the Bragg grating structures [the black lines show the contour of the structures with the same parameters as in Fig. 2(b)] with excitation wavelength at (a) resonance peak wavelength of 1556 nm, (b) off-resonance wavelength of 1650 nm.
    Fig. 3. E-field amplitude distribution of Ez component along the Bragg grating structures [the black lines show the contour of the structures with the same parameters as in Fig. 2(b)] with excitation wavelength at (a) resonance peak wavelength of 1556 nm, (b) off-resonance wavelength of 1650 nm.
    (a) Sketch of 3D simulated structure. (b) Zero-order normalized transmission of 3D slot Bragg grating structure with different numbers of air grooves on each side of the F-P cavity.
    Fig. 4. (a) Sketch of 3D simulated structure. (b) Zero-order normalized transmission of 3D slot Bragg grating structure with different numbers of air grooves on each side of the F-P cavity.
    3D-FDTD simulated zero-order normalized transmission with structure parameters as a=380 nm, Wair=260 nm, H=500 nm, Wsi=200 nm, Ws=100 nm, number of air grooves on each side of defect N=7 and varying defect size Wd.
    Fig. 5. 3D-FDTD simulated zero-order normalized transmission with structure parameters as a=380  nm, Wair=260  nm, H=500  nm, Wsi=200  nm, Ws=100  nm, number of air grooves on each side of defect N=7 and varying defect size Wd.
    3D-FDTD zero-order normalized transmission of slot Bragg grating structure with parameters of a=380 nm, Wair=260 nm, Wsi=200 nm, Ws=100 nm and the number of air grooves on each side of defect N=7 and with (a) slot etching depth H=400 nm while varying Wd=340, 360 and 380 nm. (b) Slot etching depth H=700 nm while varying Wd=320, 340, 360, and 400 nm.
    Fig. 6. 3D-FDTD zero-order normalized transmission of slot Bragg grating structure with parameters of a=380  nm, Wair=260  nm, Wsi=200  nm, Ws=100  nm and the number of air grooves on each side of defect N=7 and with (a) slot etching depth H=400  nm while varying Wd=340, 360 and 380 nm. (b) Slot etching depth H=700  nm while varying Wd=320, 340, 360, and 400 nm.
    (a) Sketch of Bragg grating with silicon height larger than LN slot height. The air grooves etching depth equal to Hsi. (b) 3D-FDTD simulated zero-order normalized transmission with structure parameters as a=380 nm, Wair=260 nm, H=500 nm, Wsi=200 nm, Ws=100 nm, number of air grooves on each side of defect N=7, Wd=380 nm, and varying the silicon height Hsi.
    Fig. 7. (a) Sketch of Bragg grating with silicon height larger than LN slot height. The air grooves etching depth equal to Hsi. (b) 3D-FDTD simulated zero-order normalized transmission with structure parameters as a=380  nm, Wair=260  nm, H=500  nm, Wsi=200  nm, Ws=100  nm, number of air grooves on each side of defect N=7, Wd=380  nm, and varying the silicon height Hsi.
    (a) 3D FDTD normalized transmission calculated by Poynting energy flux at the output of the WG with parameters of H=700 nm, a=380 nm, Wair=260 nm, Wd=340 nm, number of air grooves N=7 and with different Δn values of the LN. (b) λres versus different Δn deduced from (a).
    Fig. 8. (a) 3D FDTD normalized transmission calculated by Poynting energy flux at the output of the WG with parameters of H=700  nm, a=380  nm, Wair=260  nm, Wd=340  nm, number of air grooves N=7 and with different Δn values of the LN. (b) λres versus different Δn deduced from (a).
    WairWair/aPBG SizePBG Center
    700.2091541639
    1000.2942221613
    1400.4112501573
    1700.52321542
    2000.5882581477
    2400.7052321472
    2700.7941901441
    Table 1. PBG Size of 10 Air Grooves, a=340  nm while Varying the Value of Wair (Units in nm)
    a and WairWair/aPBG SizePBG Center
    a=350, Wair=2400.68572521508
    a=370, Wair=2600.70272741555
    a=390, Wair=2700.692961612
    a=400, Wair=2800.73041634
    a=440, Wair=3100.73421732
    Table 2. PBG Center Varying with a and Wair while Keeping Wair/a Around 0.7 (Units in nm)
    Wd (nm)λpeakTransmittance at λpeakfopt¯
    21014740.9553.27
    26015240.9543.98
    29015560.9624.03
    31015780.9613.87
    36016300.9753.24
    41016740.9782.53
    Table 3. Resonance Properties Versus the Defect Size Wd
    NλpeakTransmittance at λpeakfopt¯
    415560.9492.45
    515560.9624.03
    615540.9136.31
    715540.6685.08
    815540.3785.74
    Table 4. Resonance Properties Versus the Number of Air Grooves N
    Wentao Qiu, Huihui Lu, Fadi Issam Baida, Maria-Pilar Bernal. Ultra-compact on-chip slot Bragg grating structure for small electric field detection[J]. Photonics Research, 2017, 5(3): 212
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