Abstract <p>The response time and sensitivity in the visible spectral range of a commercial MG-32 pyroelectric detector based on the organic crystal of tetraaminodiphenyl (NZPP Vostok JSC) with a 0.5 mm thick polypropylene input window are studied. The sensor time constant is varied by connecting a capacitance <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(C\)</EquationSource> <!--OptelIns2570074Gerasimov-m1--> </InlineEquation> in the range from 2 nF to 3.8 <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570074Gerasimov-m2--> </InlineEquation>F to the feedback circuit of the receiver amplifier. With increasing capacitance in the range of 0.1–3.8 <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570074Gerasimov-m3--> </InlineEquation>F, the receiver time constant increased linearly from 0.2 to 5 ms, and at lower capacitances it reached saturation, setting a limit of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\approx\)</EquationSource> <!--OptelIns2570074Gerasimov-m4--> </InlineEquation>25 <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570074Gerasimov-m5--> </InlineEquation>s. The voltage sensitivity is tested using a diode laser (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\lambda=637\)</EquationSource> <!--OptelIns2570074Gerasimov-m6--> </InlineEquation> nm); at <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(C=0{.}1\)</EquationSource> <!--OptelIns2570074Gerasimov-m7--> </InlineEquation> <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570074Gerasimov-m8--> </InlineEquation>F, it is 3600 V W<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({}^{-1}\)</EquationSource> <!--OptelIns2570074Gerasimov-m9--> </InlineEquation>, which is 8<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\%\)</EquationSource> <!--OptelIns2570074Gerasimov-m10--> </InlineEquation> less than the sensitivity of the receiver without a polypropylene window. The equivalent noise power is virtually independent of the feedback capacitance in the range of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(C=0{.}002{-}0{.}1\)</EquationSource> <!--OptelIns2570074Gerasimov-m11--> </InlineEquation> <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mu\)</EquationSource> <!--OptelIns2570074Gerasimov-m12--> </InlineEquation>F and is <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(0{.}8\times 10^{-10}\)</EquationSource> <!--OptelIns2570074Gerasimov-m13--> </InlineEquation> W Hz<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\({}^{-1/2}\)</EquationSource> <!--OptelIns2570074Gerasimov-m14--> </InlineEquation>, while the detectivity is <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(10^{9}\)</EquationSource> <!--OptelIns2570074Gerasimov-m15--> </InlineEquation> cm W Hz<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\({}^{-1/2}\)</EquationSource> <!--OptelIns2570074Gerasimov-m16--> </InlineEquation>. These characteristics are approximately one or two orders of magnitude superior to those of other commercial pyroelectric detectors and the Golay optoacoustic cell, making the receiver under study quite promising and versatile for many applications.</p>

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Study of the Response Time and Sensitivity of the MG-32 Pyroelectric Detector with a Polypropylene Window in the Visible Range

  • V. V. Gerasimov,
  • S. E. Krasnopevtsev,
  • G. R. Turkiya,
  • D. V. Fromichev,
  • V. A. Stepanov

摘要

Abstract

The response time and sensitivity in the visible spectral range of a commercial MG-32 pyroelectric detector based on the organic crystal of tetraaminodiphenyl (NZPP Vostok JSC) with a 0.5 mm thick polypropylene input window are studied. The sensor time constant is varied by connecting a capacitance \(C\) in the range from 2 nF to 3.8 \(\mu\) F to the feedback circuit of the receiver amplifier. With increasing capacitance in the range of 0.1–3.8 \(\mu\) F, the receiver time constant increased linearly from 0.2 to 5 ms, and at lower capacitances it reached saturation, setting a limit of \(\approx\) 25 \(\mu\) s. The voltage sensitivity is tested using a diode laser ( \(\lambda=637\) nm); at \(C=0{.}1\) \(\mu\) F, it is 3600 V W \({}^{-1}\) , which is 8 \(\%\) less than the sensitivity of the receiver without a polypropylene window. The equivalent noise power is virtually independent of the feedback capacitance in the range of \(C=0{.}002{-}0{.}1\) \(\mu\) F and is \(0{.}8\times 10^{-10}\) W Hz \({}^{-1/2}\) , while the detectivity is \(10^{9}\) cm W Hz \({}^{-1/2}\) . These characteristics are approximately one or two orders of magnitude superior to those of other commercial pyroelectric detectors and the Golay optoacoustic cell, making the receiver under study quite promising and versatile for many applications.