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Quasiclassical impact theory of IR band shapes of linear molecules. / Filippov, N. N.

Proceedings of SPIE - The International Society for Optical Engineering. SPIE, 1992. p. 272-275 (Proceedings of SPIE - The International Society for Optical Engineering; Vol. 1811).

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Harvard

Filippov, NN 1992, Quasiclassical impact theory of IR band shapes of linear molecules. in Proceedings of SPIE - The International Society for Optical Engineering. Proceedings of SPIE - The International Society for Optical Engineering, vol. 1811, SPIE, pp. 272-275, Tenth All-Union Symposium on High Resolution Molecular Spectroscopy, Omsk, Russia, 2/06/91.

APA

Filippov, N. N. (1992). Quasiclassical impact theory of IR band shapes of linear molecules. In Proceedings of SPIE - The International Society for Optical Engineering (pp. 272-275). (Proceedings of SPIE - The International Society for Optical Engineering; Vol. 1811). SPIE.

Vancouver

Filippov NN. Quasiclassical impact theory of IR band shapes of linear molecules. In Proceedings of SPIE - The International Society for Optical Engineering. SPIE. 1992. p. 272-275. (Proceedings of SPIE - The International Society for Optical Engineering).

Author

Filippov, N. N. / Quasiclassical impact theory of IR band shapes of linear molecules. Proceedings of SPIE - The International Society for Optical Engineering. SPIE, 1992. pp. 272-275 (Proceedings of SPIE - The International Society for Optical Engineering).

BibTeX

@inproceedings{d720255cdb904f9db0968397c724df7a,
title = "Quasiclassical impact theory of IR band shapes of linear molecules",
abstract = "When molecular collisions are the principal line broadening mechanism the absorption at line centers and in the line wings can be calculated in impact approximation that provides the Lorentz contour for well separated lines. Apart from such lines there are regions in the IR spectra with very dense line structure (Q-branches or band heads for example) where band shape can not be expressed as the sum of Lorentzian lines. These deviations have generally been attributed to line mixing effects. We present here a theory which can be used in shape calculation of overlapped lines if the intermolecular potential is known. The quantum mechanical methods are developed for a limited number of systems and are usually too difficult to be used because of very complicated computations. Instead of this we have used the semiclassical method which can be treated in the simple model representation. The classical impact theory of shape was the basis of our method and then we modernized this theory to apply to a molecular system with discrete spectra. We shall consider here the case of the band shapes for linear molecules.",
author = "Filippov, {N. N.}",
year = "1992",
month = dec,
day = "1",
language = "English",
isbn = "081941011X",
series = "Proceedings of SPIE - The International Society for Optical Engineering",
publisher = "SPIE",
pages = "272--275",
booktitle = "Proceedings of SPIE - The International Society for Optical Engineering",
address = "United States",
note = "Tenth All-Union Symposium on High Resolution Molecular Spectroscopy ; Conference date: 02-06-1991 Through 06-06-1991",

}

RIS

TY - GEN

T1 - Quasiclassical impact theory of IR band shapes of linear molecules

AU - Filippov, N. N.

PY - 1992/12/1

Y1 - 1992/12/1

N2 - When molecular collisions are the principal line broadening mechanism the absorption at line centers and in the line wings can be calculated in impact approximation that provides the Lorentz contour for well separated lines. Apart from such lines there are regions in the IR spectra with very dense line structure (Q-branches or band heads for example) where band shape can not be expressed as the sum of Lorentzian lines. These deviations have generally been attributed to line mixing effects. We present here a theory which can be used in shape calculation of overlapped lines if the intermolecular potential is known. The quantum mechanical methods are developed for a limited number of systems and are usually too difficult to be used because of very complicated computations. Instead of this we have used the semiclassical method which can be treated in the simple model representation. The classical impact theory of shape was the basis of our method and then we modernized this theory to apply to a molecular system with discrete spectra. We shall consider here the case of the band shapes for linear molecules.

AB - When molecular collisions are the principal line broadening mechanism the absorption at line centers and in the line wings can be calculated in impact approximation that provides the Lorentz contour for well separated lines. Apart from such lines there are regions in the IR spectra with very dense line structure (Q-branches or band heads for example) where band shape can not be expressed as the sum of Lorentzian lines. These deviations have generally been attributed to line mixing effects. We present here a theory which can be used in shape calculation of overlapped lines if the intermolecular potential is known. The quantum mechanical methods are developed for a limited number of systems and are usually too difficult to be used because of very complicated computations. Instead of this we have used the semiclassical method which can be treated in the simple model representation. The classical impact theory of shape was the basis of our method and then we modernized this theory to apply to a molecular system with discrete spectra. We shall consider here the case of the band shapes for linear molecules.

UR - http://www.scopus.com/inward/record.url?scp=0026993893&partnerID=8YFLogxK

M3 - Conference contribution

AN - SCOPUS:0026993893

SN - 081941011X

T3 - Proceedings of SPIE - The International Society for Optical Engineering

SP - 272

EP - 275

BT - Proceedings of SPIE - The International Society for Optical Engineering

PB - SPIE

T2 - Tenth All-Union Symposium on High Resolution Molecular Spectroscopy

Y2 - 2 June 1991 through 6 June 1991

ER -

ID: 41434551