2013
DOI: 10.1002/lpor.201200073
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Gas in scattering media absorption spectroscopy – from basic studies to biomedical applications

Abstract: The recently introduced Gas in Scattering Media Absorption Spectroscopy (GASMAS) technique provides novel possibilities for analysis in biophotonics. Free gas in pores or cavities is monitored with narrow-band laser radiation, which can discern the gas absorptive imprints which are typically several orders of magnitude more narrow than the features of the surrounding tissue through which the diffusely scattered light emerges to the detector. Important gases monitored are oxygen and water vapour. Applications i… Show more

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Cited by 46 publications
(31 citation statements)
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References 117 publications
(149 reference statements)
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“…GASMAS data are normally expressed in an equivalent path length L eq . This value is the path length which would give rise to the same relative absorptive imprint as observed in the scattering medium . In the absence of scattering, L eq just becomes the normal geometrical path length.…”
Section: Experimental Arrangementmentioning
confidence: 92%
See 1 more Smart Citation
“…GASMAS data are normally expressed in an equivalent path length L eq . This value is the path length which would give rise to the same relative absorptive imprint as observed in the scattering medium . In the absence of scattering, L eq just becomes the normal geometrical path length.…”
Section: Experimental Arrangementmentioning
confidence: 92%
“…The GASMAS technique, which is reviewed in Ref. , has the ability to detect and characterize free gas, and the method has subsequently been applied to investigations of the sinus cavities , neonatal lungs and the femoral head . It has the potential to non‐invasively measure the concentration of oxygen also behind the eardrum, where oxygen relates to ventilation and possibly to bacterial/viral origin of infection.…”
Section: Introductionmentioning
confidence: 99%
“…The fitting equation can be obtained after using the Levenberg–Marquardt algorithm, as given by 0.12emSsample()t=P0+P1×t+P2×t2+K×Sair()t S sample and S air are the normalized GASMAS signals for light passing through the sample and the reference ambient air, respectively. K is the fitting coefficient, t is the time in the sweep of the laser frequency and P 0, P 1 and P 2 are the coefficients of a quadratic polynomial which is used for compensating the difference in base line in the measurement of the sample and the ambient air . Finally, we obtain L eq as Leq=K×Lair …”
Section: Methodsmentioning
confidence: 99%
“…The reason why this works is because the linewidth of an absorption resonance in gas molecules is several orders of magnitude less broadened by their microenvironment than absorption features of a solid or liquid material, allowing unambiguous discernment of spectral features associated with the gas. The technique of using TDLAS on scattering materials is also known as gas in scattering media absorption spectroscopy (GASMAS) . The technique has proven to be valuable in a number of medical applications by detecting gas embedded in the human sinus cavities and the mastoid bone .…”
Section: Introductionmentioning
confidence: 99%