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Quasi-molecular emission and nonadiabatic transitions : II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule. / Bichutskaya, E. N.; Devdariani, A. Z.; Zagrebin, A. L.

In: Optics and Spectroscopy (English translation of Optika i Spektroskopiya), Vol. 88, No. 2, 01.12.2000, p. 197-202.

Research output: Contribution to journalArticlepeer-review

Harvard

Bichutskaya, EN, Devdariani, AZ & Zagrebin, AL 2000, 'Quasi-molecular emission and nonadiabatic transitions: II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule', Optics and Spectroscopy (English translation of Optika i Spektroskopiya), vol. 88, no. 2, pp. 197-202. https://doi.org/10.1134/1.626772

APA

Bichutskaya, E. N., Devdariani, A. Z., & Zagrebin, A. L. (2000). Quasi-molecular emission and nonadiabatic transitions: II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule. Optics and Spectroscopy (English translation of Optika i Spektroskopiya), 88(2), 197-202. https://doi.org/10.1134/1.626772

Vancouver

Bichutskaya EN, Devdariani AZ, Zagrebin AL. Quasi-molecular emission and nonadiabatic transitions: II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule. Optics and Spectroscopy (English translation of Optika i Spektroskopiya). 2000 Dec 1;88(2):197-202. https://doi.org/10.1134/1.626772

Author

Bichutskaya, E. N. ; Devdariani, A. Z. ; Zagrebin, A. L. / Quasi-molecular emission and nonadiabatic transitions : II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule. In: Optics and Spectroscopy (English translation of Optika i Spektroskopiya). 2000 ; Vol. 88, No. 2. pp. 197-202.

BibTeX

@article{9bb06ec935e241ab9812d516cea9d5a5,
title = "Quasi-molecular emission and nonadiabatic transitions: II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule",
abstract = "Calculations are made of the quasi-molecular emission spectra formed in thermal collisions of Ca(4s4p, P-1, 4s3d, D-1) and He(1s(2), S-1(0)) atoms. The calculations are made within the framework of Demkov model [1] and in the trajectory approach on rectilinear trajectories and in the quasi-static approximation. It is shown that the Demkov model can be used for the description of the spectrum even in the case where nonadiabatic transitions are absent or negligibly weak. A rapid variation of the quasi-molecular radiative width leads to the formation of a peak in the spectrum, which is shifted to the blue wing with respect to the position of the forbidden 3(1)D --> 4(1)S(0) atomic transition. (C) 2000 MAIK {"}Nauka/Interperiodica{"}.",
keywords = "COLLISIONS",
author = "Bichutskaya, {E. N.} and Devdariani, {A. Z.} and Zagrebin, {A. L.}",
year = "2000",
month = dec,
day = "1",
doi = "10.1134/1.626772",
language = "English",
volume = "88",
pages = "197--202",
journal = "OPTICS AND SPECTROSCOPY",
issn = "0030-400X",
publisher = "Pleiades Publishing",
number = "2",

}

RIS

TY - JOUR

T1 - Quasi-molecular emission and nonadiabatic transitions

T2 - II. Ca(4s4p1P, 4s3d 1D)-He(1s2,1S0) quasi-molecule

AU - Bichutskaya, E. N.

AU - Devdariani, A. Z.

AU - Zagrebin, A. L.

PY - 2000/12/1

Y1 - 2000/12/1

N2 - Calculations are made of the quasi-molecular emission spectra formed in thermal collisions of Ca(4s4p, P-1, 4s3d, D-1) and He(1s(2), S-1(0)) atoms. The calculations are made within the framework of Demkov model [1] and in the trajectory approach on rectilinear trajectories and in the quasi-static approximation. It is shown that the Demkov model can be used for the description of the spectrum even in the case where nonadiabatic transitions are absent or negligibly weak. A rapid variation of the quasi-molecular radiative width leads to the formation of a peak in the spectrum, which is shifted to the blue wing with respect to the position of the forbidden 3(1)D --> 4(1)S(0) atomic transition. (C) 2000 MAIK "Nauka/Interperiodica".

AB - Calculations are made of the quasi-molecular emission spectra formed in thermal collisions of Ca(4s4p, P-1, 4s3d, D-1) and He(1s(2), S-1(0)) atoms. The calculations are made within the framework of Demkov model [1] and in the trajectory approach on rectilinear trajectories and in the quasi-static approximation. It is shown that the Demkov model can be used for the description of the spectrum even in the case where nonadiabatic transitions are absent or negligibly weak. A rapid variation of the quasi-molecular radiative width leads to the formation of a peak in the spectrum, which is shifted to the blue wing with respect to the position of the forbidden 3(1)D --> 4(1)S(0) atomic transition. (C) 2000 MAIK "Nauka/Interperiodica".

KW - COLLISIONS

UR - http://www.scopus.com/inward/record.url?scp=33749509201&partnerID=8YFLogxK

U2 - 10.1134/1.626772

DO - 10.1134/1.626772

M3 - Article

VL - 88

SP - 197

EP - 202

JO - OPTICS AND SPECTROSCOPY

JF - OPTICS AND SPECTROSCOPY

SN - 0030-400X

IS - 2

ER -

ID: 5240023