2010
DOI: 10.1103/physreva.81.042504
|View full text |Cite
|
Sign up to set email alerts
|

Line shapes and intensities of self-broadenedO2b1

Abstract: Line shapes and intensities of self-broadened O ) band transitions measured by cavity ring-down spectroscopyWe present high-resolution line-shape and line-intensity measurements of self-broadened Otransitions measured using the frequency-stabilized cavity ring-down spectroscopy technique under relatively low pressure conditions. We give line-shape parameters describing collisional broadening and shifting, and we treat line narrowing in terms of Dicke narrowing or the speed dependence of collisional broadening.… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

4
36
4

Year Published

2011
2011
2021
2021

Publication Types

Select...
8
1

Relationship

3
6

Authors

Journals

citations
Cited by 41 publications
(44 citation statements)
references
References 71 publications
4
36
4
Order By: Relevance
“…Specifically, the collisional narrowing frequency is given by ν nar = ηp in which η is the collisional narrowing parameter, whereas the quadratic approximation speed-dependent parameters a w and a s are independent of pressure. 64 Thus, we have utilized multi-spectrum fitting 44,45 to simultaneously fit spectra across a given range of pressures. This multi-spectrum fitting procedure produces a single value for each of the narrowing and asymmetry parameters (i.e., η, a w , and a s ).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Specifically, the collisional narrowing frequency is given by ν nar = ηp in which η is the collisional narrowing parameter, whereas the quadratic approximation speed-dependent parameters a w and a s are independent of pressure. 64 Thus, we have utilized multi-spectrum fitting 44,45 to simultaneously fit spectra across a given range of pressures. This multi-spectrum fitting procedure produces a single value for each of the narrowing and asymmetry parameters (i.e., η, a w , and a s ).…”
Section: Resultsmentioning
confidence: 99%
“…As previously demonstrated, the sensitivity and spectral fidelity of FS-CRDS make it an ideal technique for detailed study of subtle line shape effects. [36][37][38][39][40][41][42][43] Furthermore, the use of multi-spectrum fitting, [44][45][46] which simultaneously fits spectra across a wide pressure range, can enable the collisional narrowing and speed-dependent effects to be separated and quantified. Below, we present FS-CRDS line shape measurements of an air-broadened near-infrared CO 2 transition near 6360 cm −1 , and we compare our measured Lorentzian broadening parameters to literature values.…”
Section: Introductionmentioning
confidence: 99%
“…In some oxygen line-shape studies, transitions have been analysed using Galatry [19][20][21][22][23][24][25][26] or Rautian [22,23,26] profiles thus taking into account only VC but disregarding the effects of SD. The opposite assumption has also been made; the speed-dependent Voigt model being thus used while effects of VC are disregarded [22,[25][26][27]. Several alternative line shapes based on combinations of various VC and SD models have also been tested, as in [25,26].…”
Section: Introductionmentioning
confidence: 99%
“…It for instance, constituted 97% of the 144 ppm standard uncertainty published in [29]. The influence of the lineshape model on the spectroscopic determination of the Boltzmann constant has been raised by us and other groups working with O 2 and H 2 O [29,32,[40][41][42][43][44][45]. We recently carried out an extensive lineshape study at relatively high pressure in SPC, in order to enhance collisional effects and to determine the most suitable model for our data [40].…”
Section: The Lineshape Problemmentioning
confidence: 99%