• Journal of Infrared and Millimeter Waves
  • Vol. 40, Issue 1, 44 (2021)
Rui CONG*, Sheng ZHOU, Gang CHEN, Qing-Yuan CAI, Lin JIANG, and Ding-Quan LIU
Author Affiliations
  • Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
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    DOI: 10.11972/j.issn.1001-9014.2021.01.008 Cite this Article
    Rui CONG, Sheng ZHOU, Gang CHEN, Qing-Yuan CAI, Lin JIANG, Ding-Quan LIU. The effects of reflection phase shift on filtering performance of a tunable Fabry-Perot filter with a small cavity length[J]. Journal of Infrared and Millimeter Waves, 2021, 40(1): 44 Copy Citation Text show less
    Dispersion curves of refractive index and extinction coefficient of thin film materials (a) n (λ) and k (λ) of Si; (b) n (λ) and k (λ) of SiO2
    Fig. 1. Dispersion curves of refractive index and extinction coefficient of thin film materials (a) n (λ) and k (λ) of Si; (b) n (λ) and k (λ) of SiO2
    Reflection characteristics of dielectric mirrors for TFPF (a) The reflectance spectrum, (b) The reflection phase shift dispersion curve
    Fig. 2. Reflection characteristics of dielectric mirrors for TFPF (a) The reflectance spectrum, (b) The reflection phase shift dispersion curve
    Transmission spectrum of TFPF with different cavity length before and after reflection phase shift considered (a) d: 850~1 200 nm, ∆d=25 nm, ϕλ=0, m = 1, (b) d: 1 700~ 2 400 nm, ∆d=50 nm, ϕλ=0, m = 2, (c) d: 850~1 200 nm, ∆d=25 nm, ϕλ≠0, m = 0, (d) d: 1 700-2 400 nm, ∆d=50 nm, ϕλ≠0, m = 1
    Fig. 3. Transmission spectrum of TFPF with different cavity length before and after reflection phase shift considered (a) d: 850~1 200 nm, ∆d=25 nm, ϕλ=0, m = 1, (b) d: 1 700~ 2 400 nm, ∆d=50 nm, ϕλ=0, m = 2, (c) d: 850~1 200 nm, ∆d=25 nm, ϕλ0, m = 0, (d) d: 1 700-2 400 nm, ∆d=50 nm, ϕλ0, m = 1
    The relationship between peak position of passband and cavity length for TFPF (a) d: 850~1 200 nm, ∆d=25 nm; (b) d: 1 700~2 400 nm, ∆d=50 nm
    Fig. 4. The relationship between peak position of passband and cavity length for TFPF (a) d: 850~1 200 nm, ∆d=25 nm; (b) d: 1 700~2 400 nm, ∆d=50 nm
    Comparison of peak transmission for TFPF before and after reflection phase shift considered (a) d: 850~1 200 nm, ∆d=25 nm, (b) d: 17 00~2 400 nm, ∆d=50 nm
    Fig. 5. Comparison of peak transmission for TFPF before and after reflection phase shift considered (a) d: 850~1 200 nm, ∆d=25 nm, (b) d: 17 00~2 400 nm, ∆d=50 nm
    Curves of FWHM versus peak position for TFPF (a) d: 850~1 200 nm, ∆d=25 nm, (b) d: 1 700~2 400 nm, ∆d=50 nm
    Fig. 6. Curves of FWHM versus peak position for TFPF (a) d: 850~1 200 nm, ∆d=25 nm, (b) d: 1 700~2 400 nm, ∆d=50 nm
    mϕλ=0)dλp/nm(ϕλ=0λp/nm(ϕλ0Δλp/nm
    18501 7001 812.89112.89
    11 2002 4002 288.5-111.5
    21 7001 7001 768.8868.88
    22 4002 4002 332.97-67.03
    Table 1. Changes of peak position for TFPF resulting from ϕ  λ
    mϕλ=0)λp /nmFWHM ϕλ=0)FWHM ϕλ≠0)下降百分比/%
    11 812.8910.776.9435.56
    12 015.568.395.7631.34
    12 288.511.587.7133.42
    21 768.886.344.8024.29
    22 009.224.183.4118.42
    22 332.976.425.0621.18
    Table 2. Changes of FWHM for TFPF resulting from  ϕ  λ
    Rui CONG, Sheng ZHOU, Gang CHEN, Qing-Yuan CAI, Lin JIANG, Ding-Quan LIU. The effects of reflection phase shift on filtering performance of a tunable Fabry-Perot filter with a small cavity length[J]. Journal of Infrared and Millimeter Waves, 2021, 40(1): 44
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