2015
DOI: 10.1016/j.snb.2015.07.005
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Optical path length and absorption cross section optimization for high sensitivity ozone concentration measurement

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Cited by 16 publications
(11 citation statements)
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“…At the second and subsequent iterations, we perform the same procedure until the condition (7th) is satisfied [20]. The polynomial obtained at the last iteration will be considered the autofluorescence background.…”
Section: Analyzing the Spectral Properties Of Aromatic Compounds In Gases Using The Improved Methodsmentioning
confidence: 99%
“…At the second and subsequent iterations, we perform the same procedure until the condition (7th) is satisfied [20]. The polynomial obtained at the last iteration will be considered the autofluorescence background.…”
Section: Analyzing the Spectral Properties Of Aromatic Compounds In Gases Using The Improved Methodsmentioning
confidence: 99%
“…First, we set the wavelength to 257.34 nm and 279.95 nm on the gas cell simulator (For each of the absorption wavelengths we simulate results). Second, the pressure and concentration were fixed at 1013.25mbar and 950ppm respectively [9], [12]. Third, values of optical path-length were then inserted beginning from 0.75cm -130cm while the temperature was then varied from 100K -350K for each optical path-length.…”
Section: Simulation and Methodologymentioning
confidence: 99%
“…Of the afore mention bands, the Hartley band has the strongest absorption of light in the UV spectrum, hence a high OACS [10] Therefore, ozone gas concentration in the atmosphere could be efficiently measured in the Hartley band (between 200 to 300 nm). 257.34 nm [11] and 279.95 nm [12] being in the Hartley band have also shown strong absorption cross section of ozone in the UV. To a large extent, in the Hartley band, ozone gas has a unique property that allows very strong absorption of UV radiation.…”
Section: Introductionmentioning
confidence: 91%
“…However, the sensor saturation may occur, which may limit the sensitivity and linearity. Marcus et al [20] investigated the sensor saturation and derived equations based on Beer–Lambert law for optimized transmittance, optical path length, and absorption cross-section for a specific range of ozone concentration to prevent sensor saturation. The optimized optical path length, l op and optimized cross-section σ op for ozone concentrations c 1 and c 2 were derived as expressed as, lop=106 R T false(lnc1lnc2false)σ NAP (c1c2); σop=106 R T false(lnc1lnc2false)l NAP (c1c2) whereas c is the concentration of an analyte in ppm; σ is absorption cross-section in m 2 -molecule −1 ; T is absolute temperature in K ; P is pressure in atm; R is ideal gas constant, 8.205746 × 10 −5 atm-m 3 mol −1 - K −1 ; N A is Avogadro’s constant, 6.02214199 × 10 23 molecule-mol −1 .…”
Section: Uv Spectrophotometrymentioning
confidence: 99%