Gas analysis is essential in various industries, providing critical insights for environmental monitoring, medical diagnostics, and industrial process control [1]. This article examines the significant advancements brought by Quantum Cascade Lasers (QCLs) in enhancing gas analysis techniques. By meeting stringent requirements for sensitivity, selectivity, speed, and robustness, QCLs are instrumental in accurately detecting and quantifying gases in complex environments. We will explore the applications and advantages of optical gas sensing technologies, particularly in challenging scenarios where precision and reliability are paramount.
Gas analysis is vital for environmental applications, enabling the quantification of greenhouse gas (GHG) emissions and their geographical distribution. Industries such as agriculture, manufacturing, and transportation rely on accurate gas measurements to assess their impact on climate change and comply with environmental regulations.
In the medical field, precise gas analysis is indispensable. A prominent example is capnography, a non-invasive technique that continuously measures carbon dioxide (CO2) concentration in a patient's breath. This real-time data is critical for assessing ventilatory status, confirming endotracheal tube placement, and monitoring patients during sedation or anesthesia.
In industrial settings, gas analysis is crucial for process monitoring and control, ensuring quality assurance, yield optimization, and regulatory compliance. The technologies utilized in this arena are collectively referred to as Process Analytical Technologies (PAT), which enhance operational efficiency and safety.
While several gas sensing technologies are available, optical technologies have some distinct advantages over the others. Optical gas sensing techniques rely on spectroscopy principles, using the unique absorption characteristics of gases for their quantification [Fig. 1]. These methods do not require consumables such as chemicals or adsorbents, resulting in high energy efficiency, long measurement life and low cost per test.
Furthermore, optical gas sensing technologies can be seamlessly integrated into automated systems used in applications that require continuous operation. In recent years, optical gas sensing technologies has seen a surge in popularity. This is due to advancements in light source and detector technologies operating in the near- and mid-infrared regions [2] (NIR and MIR) of the optical spectrum where gas absorption is strong.
Figure 1: Single pass gas cell used for optical gas sensing by absorption spectroscopy.
Choosing the right source or detector for optical gas sensing hinges on the application's specific demands. For process control and monitoring – one of the most challenging gas sensing contexts – the following criteria are imperative:
High Sensitivity
Ability to detect trace gas concentrations.
High Selectivity
Accurate quantification of individual gases within complex mixtures.
Rapid Measurements
High throughput while maintaining accuracy.
Robustness
Reliability and accuracy maintained over extended periods.
Failure to meet these requirements can result in substantial losses, especially in large-scale industrial operations that depend on reliable process control and monitoring. In scenarios involving toxic or polluting gases, non-compliance with emission regulations can lead to severe penalties.
Quantum cascade lasers (QCLs) are some of the best MIR light sources for analytical applications. These are small semiconductor lasers that can be operated in both continuous and pulsed modes. Unlike most MIR sources, the linewidth of QCLs is extremely narrow (< 1 MHz), which is required for a high degree of spectral selectivity in applications like gas sensing, where absorption peaks in the MIR region are narrow. In a mixture of gases, the absorption bands of gases in a mixture often lie close together spectrally. To distinguish one from the other, narrow-linewidth light sources like QCLs are the appropriate choice.
According to Beer-Lambert’s law, gas sensing uses absorption spectroscopy whose signal strength depends on the concentration of the gas, light intensity, and the interaction path length [3]. Being lasers, QCLs’ output can be easily collimated into a high-intensity beam, which is an advantage in sensing low concentrations (a few parts per million). Moreover, the collimated beam also makes it easy to design multipass gas cells [Fig. 2], also known as Herriott cells. The purpose of Herriott cells is to increase the interaction path length. The more collimated a light source is, the easier it is to increase the number of passes in a Herriott cell, eventually heightening the sensitivity. Therefore, QCLs have a twofold advantage over non-laser-type MIR sources in terms of sensitivity.
Signal strength in absorption spectroscopy
∞ Conc of target gas × Intensity of light × Interaction path length
The high sensitivity of QCL-based gas analysis, combined with fast, low-noise detectors, shortens acquisition times. This enables frequent and precise measurements necessary for process control, a process dependent on input and output flow rates. When high gas flow rates are required, equally fast gas analysis methods are required for effective monitoring and control. QCLs’ fast response allows fast switching and high frequency modulation, further aiding high speed gas sensing.
Figure 2: Multipass gas cell used for optical gas sensing by absorption spectroscopy.
QCLs are robust semiconductor lasers. When coupled with an appropriate thermoelectric cooling mechanism and a low noise power supply, they maintain wavelength stability and operational efficiency under demanding conditions with little intervention. These factors make QCLs one of the best MIR sources for gas sensing in process control and monitoring.
With over a decade of experience, Hamamatsu Photonics provides quantum cascade lasers (QCLs) for process control and monitoring applications. The company has continually enhanced its QCL product line, offering improved packaging options, compact sizes, integrated thermoelectric cooling mechanisms, and a variety of wavelength selections. While a limited set of QCL wavelengths is listed online [4], custom options between 4-12 μm are available on request. Additionally, Hamamatsu offers a diverse selection of RoHS-compliant mid-infrared (MIR) detectors [5] available in various packages and spectral ranges.
Hamamatsu stands out for its commitment to developing QCL technology and accompanying MIR detection solutions.
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