• Advanced Photonics Nexus
  • Vol. 2, Issue 4, 046002 (2023)
Zheng Ge1、2, Zhi-Yuan Zhou1、2、*, Jing-Xin Ceng3, Li Chen1、2, Yin-Hai Li1、2, Yan Li1、2, Su-Jian Niu1、2, and Bao-Sen Shi1、2、*
Author Affiliations
  • 1University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, China
  • 2University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, China
  • 3Science and Technology on Electro-Optical Information Security Control Laboratory, Tianjin, China
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    DOI: 10.1117/1.APN.2.4.046002 Cite this Article Set citation alerts
    Zheng Ge, Zhi-Yuan Zhou, Jing-Xin Ceng, Li Chen, Yin-Hai Li, Yan Li, Su-Jian Niu, Bao-Sen Shi. Thermal camera based on frequency upconversion and its noise-equivalent temperature difference characterization[J]. Advanced Photonics Nexus, 2023, 2(4): 046002 Copy Citation Text show less

    Abstract

    We present a scheme for estimating the noise-equivalent temperature difference (NETD) of frequency upconversion detectors (UCDs) that detect mid-infrared (MIR) light. In particular, we investigate the frequency upconversion of a periodically poled crystal based on lithium niobate, where an MIR conversion bandwidth of 220 nm can be achieved in a single-poled period by a special design. Experimentally, for an MIR radiating target at a temperature of 95°C, the NETD of the device was estimated to be 56 mK with an exposure time of 1 s. Meanwhile, a direct measurement of the NETD was performed utilizing conventional methods, which resulted in 48 mK. We also compared the NETD of our UCD with commercially available direct MIR detectors. We show that the limiting factor for further NETD reduction of our device is not primarily from the upconversion process and camera noise but from the limitations of the heat source and laser performance. Our detectors have good temperature measurement performance and can be used for a variety of applications involving temperature object identification and material structure detection.
    ϕeλ=MeλA0Ωπτ(λ),

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    Meλ(λ,T)=2πhc2λ5·1ehcλkT1,

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    ϕeλT=MeλTΩπA0τ(λ).

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    (δNS)T=MeλTΩπA0τ(λ)R0(λ)=ΩπA0τ(λ)NnNEP(λ)MeλT.

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    NEP=σRprΔf=σRηupηdethνMIRΔf=σRhνMIRηupηdetΔf,

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    NsTΔNsΔT=ωA0NnπNEP0MeλTτ(λ)dλ.

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    ΔNsNn=ΔTωA0πNEP0MeλTτ(λ)dλ.

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    NETD=πNEPΩA00MeλTτ(λ)dλ=πNEPΩA0τ0MeλTdλ=πNEPΩA0τhckTB2λ1λ2Meλ(TB)λdλ,

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    ηup=Pup/hνupPMIR/hνMIR=PupνMIRPMIRνup=PupνMIRλ1λ2ϕeλdλνup,

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    ηdet==PdetPup=x¯RhνupPup,

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    NETD=σRkTB2λ1λ2Meλ(TB)dλx¯Rhcλ1λ2Meλ(TB)λdλ.

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    Zheng Ge, Zhi-Yuan Zhou, Jing-Xin Ceng, Li Chen, Yin-Hai Li, Yan Li, Su-Jian Niu, Bao-Sen Shi. Thermal camera based on frequency upconversion and its noise-equivalent temperature difference characterization[J]. Advanced Photonics Nexus, 2023, 2(4): 046002
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