• Acta Optica Sinica
  • Vol. 40, Issue 8, 0811002 (2020)
Kaiyu Yang*, Ning Jin**, Ling Cao, and Man Xu
Author Affiliations
  • Institute of Night-Vision Technology, Kunming Institute of Physics, Kunming, Yunnan 650223, China
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    DOI: 10.3788/AOS202040.0811002 Cite this Article Set citation alerts
    Kaiyu Yang, Ning Jin, Ling Cao, Man Xu. Optimization Design of Stop Aperture Shape for Uncooled Infrared Detector[J]. Acta Optica Sinica, 2020, 40(8): 0811002 Copy Citation Text show less
    Schematic of stray radiation and stop aperture of uncooled infrared detector
    Fig. 1. Schematic of stray radiation and stop aperture of uncooled infrared detector
    “Pot cover effect” caused by stray radiation of uncooled infrared detector
    Fig. 2. “Pot cover effect” caused by stray radiation of uncooled infrared detector
    Transmission of radiation energy between two surfaces
    Fig. 3. Transmission of radiation energy between two surfaces
    Spatial rectangular coordinate system for calculation of stray radiation transmission path
    Fig. 4. Spatial rectangular coordinate system for calculation of stray radiation transmission path
    Stray radiation emissive region model
    Fig. 5. Stray radiation emissive region model
    Variable elements for describing stop aperture shape
    Fig. 6. Variable elements for describing stop aperture shape
    Flow chart for optimizing stop aperture shape by interval exhaustion method
    Fig. 7. Flow chart for optimizing stop aperture shape by interval exhaustion method
    Dimensions (unit:mm). (a) Radiant surface of case; (b) plane of front baffle
    Fig. 8. Dimensions (unit:mm). (a) Radiant surface of case; (b) plane of front baffle
    Stop aperture shape after optimization
    Fig. 9. Stop aperture shape after optimization
    Distribution of stray irradiance along diagonal line of FPA. (a) Without stop; (b) with stop
    Fig. 10. Distribution of stray irradiance along diagonal line of FPA. (a) Without stop; (b) with stop
    Distribution of stray irradiance on FPA. (a) Without stop; (b) with stop
    Fig. 11. Distribution of stray irradiance on FPA. (a) Without stop; (b) with stop
    Type of dataData input
    Data of FPAArray size of 640×512, pitch of 17 μm, wavelength of 8--12 μm
    Data of windowSize of 16.9 mm×14.7 mm, d=1 mm, n=4.0043
    Radiation properties of structural partsEmissivity of 80%, absorption of 80%, reflectivity of 20%, temperature of 300 K
    Distance between stop and FPA0.8 mm
    Distance between radiant surface of case and FPA1.15 mm
    Distance between plane of front baffle and FPA7.35 mm
    Initial shape of stop apertureRectangle of 11.20 mm×9 mm
    Restriction range of stop apertureBetween two concentric rectangles of 11.20 mm×9 mm and 16.9 mm×14.7 mm
    Table 1. Data input for optimization of shape of stop aperture
    Kaiyu Yang, Ning Jin, Ling Cao, Man Xu. Optimization Design of Stop Aperture Shape for Uncooled Infrared Detector[J]. Acta Optica Sinica, 2020, 40(8): 0811002
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