Laser & Optoelectronics Progress, Volume. 56, Issue 20, 202411(2019)
Magneto-Optical Surface Plasmon Resonance and Refractive Index Sensor Based on Au/Ce∶YIG/TiN Structure
Fig. 2. Reflectivity as a function of r, h, p, θ, and wavelength. (a) Reflectivity versus r when h=30 nm, p=600 nm, and θ=45°; (b) reflectivity versus h when r=70 nm, p=600 nm, and θ=45°;(c) reflectivity versus p when r=70 nm, h=30 nm, and θ=45°;(d) reflectivity versus θ when r=70 nm, h=30 nm, and p=650 nm
Fig. 3. Cross-section of device and magnetic field H distributions under different structural parameters. (a) Cross-section of xoz plane of device when r=100 nm; (b) SPP mode;(c) LSPR mode; (d) coupling mode when r=70 nm
Fig. 4. TMOKE as a function of r, h, p, θ, and wavelength. (a) TMOKE versus r when h=30 nm, p=600 nm, and θ=45°; (b) TMOKE versus h when r=70 nm, p=600 nm, and θ=45°;(c) TMOKE versus p when r=70 nm, h=30 nm, and θ=45°; (d) TMOKE versus θ when r=70 nm, h=30 nm, and p=650 nm
Fig. 5. Refractive index sensing performance of the device. (a) Change of TMOKE at different refractive indexes; (b) change of peak position at different refractive indexes
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Huili Wang, Jun Qin, Tongtong Kang, Yan Zhang, Lixia Nie, Wansen Ai, Yanfang Li, Lei Bi. Magneto-Optical Surface Plasmon Resonance and Refractive Index Sensor Based on Au/Ce∶YIG/TiN Structure[J]. Laser & Optoelectronics Progress, 2019, 56(20): 202411
Category: Optics at Surfaces
Received: Jan. 28, 2019
Accepted: Apr. 25, 2019
Published Online: Oct. 22, 2019
The Author Email: Lei Bi (bilei@uestc.edu.cn)