Abstract

In this paper we propose multispectrum rotational states distribution thermometry as an optical method for primary thermometry. It relies on a global fitting of multiple absorption lines of the same band at different pressures. The approach allows leveraging both the temperature-dependent Doppler width and the temperature-dependent distribution of line intensities across the ro-vibrational band. We provide a proof-of-principle demonstration of the approach on the 3ν1 + ν3 band of CO2, for which several accurate line-strength models of both theoretical and experimental origin are available for the global fitting. Our experimental conditions do not allow to test the methodology beyond a combined uncertainty of 530 ppm, but the comparative analysis between different line-strength models shows promise to reduce the error budget to few tens of ppm. As compared to Doppler-broadening thermometry, the approach is advantageous to mitigate systematic errors induced by a wrong modelling of absorption line-shapes and to reduce, for a given experimental dataset, the statistical uncertainty by a factor of 2. When applied in a reverse way, i.e. using a gas of known temperature, the approach becomes a stringent testbed for the accuracy of the adopted line-strength model.

Highlights

  • 25 August 2020R Gotti1,5 , M Lamperti , D Gatti , S Wojtewicz, T Puppe, Y Mayzlin, B Alsaif, J Robinson-Tait, F Rohde, R Wilk, P Leisching, W G Kaenders, P Laporta and M Marangoni

  • The microscopic thermal energy, given by the product of the Boltzmann constant with the thermodynamic temperature (T ), influences several macroscopic parameters of different physical systems

  • We have proposed multispectrum rotational states distribution thermometry (MRDT) as an optical approach to primary thermometry, based on the simultaneous analysis of an ensemble of transitions of the same absorption band at different pressures

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Summary

25 August 2020

R Gotti1,5 , M Lamperti , D Gatti , S Wojtewicz, T Puppe, Y Mayzlin, B Alsaif, J Robinson-Tait, F Rohde, R Wilk, P Leisching, W G Kaenders, P Laporta and M Marangoni. Poland 3 TOPTICA Photonics AG, Lochhamer Schlag 19, 82166 Grafelfing, Germany 4 Clean Combustion Research Center, King Abdullah University for Science and Technology, Thuwal, Saudi Arabia 5 Authors to whom any correspondence should be addressed

Introduction
The optical thermometer
Temperature model and fitting procedure
Experiments and results
Conclusions

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