
FOLLOWUS
1. National Key Laboratory of Laser Spatial Information, Harbin Institute of Technology,Harbin,China,150001
2. Zhengzhou Research Institute, Harbin Institute of Technology,Zhengzhou,China,450000
纸质出版日期:2025
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High-Stability and Fast Calibration-Free Temperature Measurement Based on Light-Induced Thermoelastic Spectroscopy[J]. 超快科学(英文), 2025,5(1).
Xiaonan Liu, Shunda Qiao, Ying He, et al. High-Stability and Fast Calibration-Free Temperature Measurement Based on Light-Induced Thermoelastic Spectroscopy[J]. Ultrafast science, 2025, 5(1).
High-Stability and Fast Calibration-Free Temperature Measurement Based on Light-Induced Thermoelastic Spectroscopy[J]. 超快科学(英文), 2025,5(1). DOI: 10.34133/ultrafastscience.0083.
Xiaonan Liu, Shunda Qiao, Ying He, et al. High-Stability and Fast Calibration-Free Temperature Measurement Based on Light-Induced Thermoelastic Spectroscopy[J]. Ultrafast science, 2025, 5(1). DOI: 10.34133/ultrafastscience.0083.
In this paper
a series of calibration-free temperature measurement methods based on light-induced thermoelastic spectroscopy (LITES) are proposed for the first time. These techniques utilize the steady-state and transient response characteristics of the quartz tuning fork (QTF)
namely
the calibration-free LITES (CF-LITES) and calibration-free heterodyne LITES (CF-H-LITES) methods. Four methods
first harmonic (1f) difference signal to normalize the second harmonic (2f) fundamental signal (method I
2ffund/1fdiff)
1f overtone signal to normalize the 2f fundamental signal (method II
2ffund/1fover)
1f heterodyne difference signal to normalize the 2f heterodyne fundamental signal (method III
2f-Hfund/1f-Hdiff)
and 1f heterodyne overtone signal to normalize the 2f heterodyne fundamental signal (method IV
2f-Hfund/1f-Hover)
for simultaneously detecting 1f and 2f within the frequency response range of the QTF are proposed to achieve calibration-free measurement. A self-designed T-shaped QTF with low fundamental and overtone frequencies was used to increase the energy accumulation time
thereby enhancing the sensor signal level. A 3-stage tube furnace was adopted to verify the performance of these 4 methods. Experimental results showed that the errors for the 4 methods were less than 4%
with a standard deviation below 11 °C. Furthermore
the calibration-free method
which employs normalization of the 2f signal with the 1f signal
effectively mitigates the impact of laser beam jitter and power fluctuations on detection performance. A superior performance can be obtained by adopting the CF-H-LITES technique based on method IV. It not only has excellent detection performance but also reduces the measurement period to 4 s
which is about 5 times faster. This development shows substantial promise for expanding the application of the CF-LITES and CF-H-LITES techniques in harsh environments.
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