As part of the development of a spectrally uniform room-temperature absolute radiometer, we have studied the electrical noise of several bulk chip thermistors in order to estimate the noise floor and optical dynamic range. Understanding the fundamental limits of the temperature sensitivity leads inevitably to studying the noise background of the complex electro-thermal system. To this end, we employ a measurement technique based on alternating current synchronous demodulation. Results of our analysis show that the combination of a low-current noise Junction Field Effect Transistor (JFET) preamplifier together with chip thermistors is optimal for our purpose, yielding a root mean square noise temperature of 2.8 μK in the frequency range of 0.01 Hz to 1 Hz.
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February 2017
Research Article|
February 13 2017
Noise characteristics of thermistors: Measurement methods and results of selected devices
Ivan Ryger;
Ivan Ryger
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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Dave Harber;
Dave Harber
2
Laboratory for Atmospheric and Space Physics
, Boulder, Colorado 80303-7814, USA
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Michelle Stephens
;
Michelle Stephens
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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Malcolm White;
Malcolm White
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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Nathan Tomlin
;
Nathan Tomlin
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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Matthew Spidell;
Matthew Spidell
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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John Lehman
John Lehman
1
National Institute of Standards and Technology
, Boulder, Colorado 80305, USA
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Rev. Sci. Instrum. 88, 024707 (2017)
Article history
Received:
October 12 2016
Accepted:
January 29 2017
Citation
Ivan Ryger, Dave Harber, Michelle Stephens, Malcolm White, Nathan Tomlin, Matthew Spidell, John Lehman; Noise characteristics of thermistors: Measurement methods and results of selected devices. Rev. Sci. Instrum. 1 February 2017; 88 (2): 024707. https://doi.org/10.1063/1.4976029
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