2020
DOI: 10.1088/1361-6501/ab58a6
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Developments towards an industrial Johnson noise thermometer

Abstract: In this paper we present new developments in our practical, driftfree Johnson noise thermometer as it moves from a proofofprinciple prototype towards a practical implementation to become a viable primary thermometer for industrial applications. We will discuss bandwidth optimisation to obtain the lowest possible uncertainty of temperature measurements. The concept of weighting the crosscorrelation frequency bins to improve the uncertainty will be introduced and it will be shown that this can decrease the measu… Show more

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Cited by 14 publications
(8 citation statements)
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“…One of the aforementioned techniques, the superposition thermometer, has been commercially developed by Metrosol 5 in collaboration with the National Physical Laboratory (NPL), UK (see figure 6) [56][57][58]. It uses pseudo random current injection for the calibration signal, which can be separated from Johnson noise in the frequency domain.…”
Section: Jntmentioning
confidence: 99%
“…One of the aforementioned techniques, the superposition thermometer, has been commercially developed by Metrosol 5 in collaboration with the National Physical Laboratory (NPL), UK (see figure 6) [56][57][58]. It uses pseudo random current injection for the calibration signal, which can be separated from Johnson noise in the frequency domain.…”
Section: Jntmentioning
confidence: 99%
“…Such an approach will be needed to make autonomous production truly a reality. Such approaches could be through practical Johnson Noise Thermometry (where practical demonstrator devices already exist) [69,70] and in the longer-term small-scale Doppler Broadening Thermometry [71,72] as well as other photonic based approaches [73].…”
Section: Future Temperature Realisation and Disseminationmentioning
confidence: 99%
“…To turn one of these into a practical, commercially available reality, NPL has been collaborating with Metrosol Limited to develop a practical Johnson noise thermometer [8][9][10]. The Johnson noise voltage is related to temperature by Nyquist's relation <VT 2 > = 4kTRf, where <VT 2 > is the mean squared Johnson noise voltage, k is the Boltzmann constant, R is the sensor resistance and f is the frequency bandwidth which is a function of the sensing electronics and cables.…”
Section: Practical Primary Thermometrymentioning
confidence: 99%