Abstract

Photothermal spectroscopy (PTS) is a technique used for determining the composition of liquids, solids and gases. In PTS, the sample is illuminated with a radiation source, and the thermal response of the analyte (e.g., refractive index) is analyzed to gain information about its content. Recent advances in this unique method of detecting gaseous samples show that photothermal gas spectroscopy can be an interesting alternative to commonly used absorption techniques. Moreover, if designed properly, sensors using PTS detection technique can not only reach sensitivities comparable with other, more complex techniques, but can significantly simplify the design of the sensor. In this review, recent developments in photothermal spectroscopy of gases will be summarized and discussed.

Highlights

  • Photothermal spectroscopy (PTS) is a group of spectroscopy techniques commonly used to measure thermal characteristics and optical absorption of samples [1,2,3]

  • As presented in this review, PT gas detection can be accomplished in numerous dissimilar configurations, encouraging researchers to search for novel, yet unpublished, methods of utilizing the PT effect for precise and selective trace gas analysis

  • FP interferometric readout of the PT-induced refractive index (RI) modulation has proven to be very sensitive and foremost miniature. With proper design, this configuration is capable of reaching strong absorption lines of molecules located in the mid-infrared wavelength region

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Summary

Introduction

Photothermal spectroscopy (PTS) is a group of spectroscopy techniques commonly used to measure thermal characteristics and optical absorption of samples (solids, liquids or gases) [1,2,3]. Absorption of the molecules causes a reduction of the intensity, which is detected by a photodiode and signal-processed to determine the gas concentration or other properties of the gas (e.g., pressure, temperature, velocity) [9] As this method usually relies on calculating the difference between the input light intensity and the light absorbed by the sample, the performance and accuracy of the sensor is limited especially in the case of small absorption and by reflections and scattering effects usually present in such systems. To PAS, the PTS signal decreases with higher pump laser modulation frequencies [17] This is a direct result of the limited thermal response time of the gas molecules and has been thoroughly explained in Reference [18].

First Experimental Verification of PTS Gas Sensors
Optical Heterodyne Gas Spectrometer
Homodyne Hydrazine Detector with Folded Jamin Interferometer
Fiber-Based Photothermal Gas Sensors
Fiber-Based Heterodyne Detection of PTS Signals
Spatial Gas Sample Localization in an Fiber-Based PTS Sensor
PTS in Hollow-Core Fibers
Pulsed PTS in Hollow-Core Fibers
Intra-Cavity PTS Gas Sensors
PTS in an Intracavity He-Ne Laser Configuration
All-Fiber Intracavity PT Gas Sensor
Intracavity PT Detection in a Mode-Locked Laser Configuration
Fabry-Perot-Based PTS Gas Sensors
Fabry-Perot PT Gas Sensor with 2f Modulation
Balanced Detection Fabry-Perot PT Gas Sensor
Conclusions
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