Comparison of CRDS to ICL-PAS and phase-shift CRDS spectroscopies for the absolute intensities of C–H (Δ vCH=6) overtone absorptions
Cavity ring-down spectroscopy (CRDS) has been used to obtain the visible overtone spectra (Δ v CH=6) of neo-pentane, C(CH 3) 4, propane, C 3H 8, and n-butane, C 4H 10, yielding absolute f-values for the transitions to better than 3%. For the neo-pentane overtone intensity, comparison with a recent m...
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Published in | Chemical physics letters Vol. 366; no. 3; pp. 383 - 389 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Amsterdam
Elsevier B.V
10.12.2002
Elsevier Science |
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Abstract | Cavity ring-down spectroscopy (CRDS) has been used to obtain the visible overtone spectra (Δ
v
CH=6) of
neo-pentane, C(CH
3)
4, propane, C
3H
8, and
n-butane, C
4H
10, yielding absolute
f-values for the transitions to better than 3%. For the
neo-pentane overtone intensity, comparison with a recent measurement using intra-cavity laser photoacoustic spectroscopy (ICL-PAS) provides favourable agreement, with improved precision. Being absolute this value may be used as a standard for relative intensity measurements obtained by ICL-PAS. The measured propane and
n-butane overtone intensities, when compared to recent work using phase-shift CRDS, indicate a lack of agreement to quoted uncertainties. |
---|---|
AbstractList | Cavity ring-down spectroscopy (CRDS) has been used to obtain the visible overtone spectra (Δ
v
CH=6) of
neo-pentane, C(CH
3)
4, propane, C
3H
8, and
n-butane, C
4H
10, yielding absolute
f-values for the transitions to better than 3%. For the
neo-pentane overtone intensity, comparison with a recent measurement using intra-cavity laser photoacoustic spectroscopy (ICL-PAS) provides favourable agreement, with improved precision. Being absolute this value may be used as a standard for relative intensity measurements obtained by ICL-PAS. The measured propane and
n-butane overtone intensities, when compared to recent work using phase-shift CRDS, indicate a lack of agreement to quoted uncertainties. |
Author | Brooks, R.L DeMille, S Tanner, R.M deLaat, R.H Westwood, N.P.C |
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CitedBy_id | crossref_primary_10_1080_00268970902881987 crossref_primary_10_1016_j_cplett_2006_09_007 crossref_primary_10_1016_j_cplett_2004_10_081 crossref_primary_10_1021_acs_jpca_5b05884 crossref_primary_10_7498_aps_68_20182262 crossref_primary_10_1016_j_cplett_2004_06_102 crossref_primary_10_1021_ac0491253 crossref_primary_10_1139_p05_054 |
Cites_doi | 10.1021/jp0209493 10.1021/ar00144a001 10.1016/0009-2614(91)80151-M 10.1063/1.458993 10.1139/v01-015 10.1080/014423500750040627 10.1016/S0009-2614(00)01466-4 10.1063/1.443925 10.1016/0009-2614(96)01048-2 10.1063/1.450527 10.1039/a707686j 10.1063/1.1139895 10.1016/0009-2614(85)80286-4 10.1139/p01-042 |
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Keywords | Vibrational transition Butane Visible spectra Laser spectroscopy Hydrocarbons Absorption spectra Experimental study Pentane Propane Organic compounds |
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Snippet | Cavity ring-down spectroscopy (CRDS) has been used to obtain the visible overtone spectra (Δ
v
CH=6) of
neo-pentane, C(CH
3)
4, propane, C
3H
8, and
n-butane,... |
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SourceType | Aggregation Database Index Database Publisher |
StartPage | 383 |
SubjectTerms | Atomic and molecular physics Biological and medical applications Exact sciences and technology Fundamental areas of phenomenology (including applications) Laser spectroscopy Molecular properties and interactions with photons Molecular spectra Optics Physics Visible spectra |
Title | Comparison of CRDS to ICL-PAS and phase-shift CRDS spectroscopies for the absolute intensities of C–H (Δ vCH=6) overtone absorptions |
URI | https://dx.doi.org/10.1016/S0009-2614(02)01616-0 |
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