Abstract

Spectral characteristics of specific detectivity D<SUP>*</SUP>((lambda) <SUB>m</SUB>) and noise equivalent temperature difference NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) were calculated for background noise limited thermal detectors with restricted spectral range ((lambda) <SUB>m</SUB> - cut-off wavelength). In the actual spectral range ((lambda) <SUB>m</SUB>&lt;15 micrometers ) thermal detectors are able to ensure the same values of D<SUP>*</SUP>((lambda) <SUB>m</SUB>) and NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) as for quantum detectors. NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) and D<SUP>*</SUP>((lambda) <SUB>m</SUB>) values are shown to be connected by `kT<SUP>2</SUP>-rule': NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) - (root)2kT<SUP>2</SUP>D<SUP>*</SUP>((lambda) <SUB>m</SUB>). It was accentuated that this rule may be applied to quantum photodetectors but with some definitions. The approximations were offered permitting to calculate values of D<SUP>*</SUP>((lambda) <SUB>m</SUB>) and NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) in all spectral ranges with the accuracy of not worse than 2%. It was shown that as D<SUP>*</SUP>((lambda) <SUB>m</SUB>) of an ideal thermal detector with a cold filter increases the cooling temperature necessary for achievement of theoretical limited values of D<SUP>*</SUP>((lambda) <SUB>m</SUB>) and NETD<SUP>*</SUP>((lambda) <SUB>m</SUB>) also increases. Such a behavior is opposite to that known for quantum photodetectors.

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