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Photoacoustic Spectroscopy is a technique, based on the measurements of the acoustic effects, emerging during absorption of light by the analysed matter (gas). Upon radiation of gas by light, the temperature of gas increases, leading to a periodic expansion and contraction of gas volume, synchronous with the modulation frequency of radiation. This generates a pressure wave (sound) that can be detected by the microphone (Dumitras et al. 2007). Intensity of generated sound is proportional to the light intensity, and that is why laser light sources are widely applied in this technique. Even though the technique was applied for atmospheric measurements more than 30 years ago (Meyer, Sigrist 1990), the technology is significantly advancing due to the development of new laser sources (Gondal et al. 2012; Wang and Wang 2016) and other parts of experimental set-ups, such as resonators (Tavakoli et al. 2010).
 
Photoacoustic Spectroscopy is a technique, based on the measurements of the acoustic effects, emerging during absorption of light by the analysed matter (gas). Upon radiation of gas by light, the temperature of gas increases, leading to a periodic expansion and contraction of gas volume, synchronous with the modulation frequency of radiation. This generates a pressure wave (sound) that can be detected by the microphone (Dumitras et al. 2007). Intensity of generated sound is proportional to the light intensity, and that is why laser light sources are widely applied in this technique. Even though the technique was applied for atmospheric measurements more than 30 years ago (Meyer, Sigrist 1990), the technology is significantly advancing due to the development of new laser sources (Gondal et al. 2012; Wang and Wang 2016) and other parts of experimental set-ups, such as resonators (Tavakoli et al. 2010).
  
<div class="tablecaption" id="table16">TABLE 16 STRENGTHS AND LIMITATIONS OF LPAS</div>
+
TABLE 16 STRENGTHS AND LIMITATIONS OF LPAS
{| class="wikitable"
 
|-
 
! scope="col" | Strengths
 
! scope="col" | Limitations
 
|-
 
! scope="row" | High sensitivity (ppb)
 
| Strict requirements for laser source (power, tuning range, band width, )
 
|-
 
! scope="row" | Selective excitation of several species
 
| sound detecting system is sensitive to the environmental noise
 
|-
 
! scope="row" | Easy to detect large molecules
 
|  Hard to detect small molecules
 
|-
 
! scope="row" | Due to photo-thermal mechanism, LPAS is useful for transparent samples where the light absorption is small
 
|
 
|}
 
Producers of LPAS technique are listed in table 17
 
  
<div class="tablecaption" id="table17">TABLE 17 PRODUCERS OF DEVICES FOR LPAS</div>
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TABLE 17 PRODUCERS OF DEVICES FOR LPAS
{| class="wikitable"
 
! scope="col" | Company
 
! scope="col" | website
 
|-
 
! scope="row" | GASERA
 
|  http://www.gasera.fi/
 
|-
 
! scope="row" | LumaSense TECHNOLOGIES
 
|  https://www.lumasenseinc.com/
 
|-
 
! scope="row" | California Analytical Instruments, Inc.
 
|  http://www.gasanalysers.com/
 
|-
 
! scope="row" | MirSense
 
|  http://mirsense.com/
 
|-
 
! scope="row" | AEROVIA
 
|  https://aerovia.fr/
 
|}
 
  
 
===2.1.4 Development of GHG sensors market===
 
===2.1.4 Development of GHG sensors market===

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