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Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential. / Golubkov, G. V.; Devdariani, A. Z.; Golubkov, M. G.

в: Journal of Experimental and Theoretical Physics, Том 95, № 6, 01.12.2002, стр. 987-997.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Golubkov, GV, Devdariani, AZ & Golubkov, MG 2002, 'Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential', Journal of Experimental and Theoretical Physics, Том. 95, № 6, стр. 987-997. https://doi.org/10.1134/1.1537291

APA

Golubkov, G. V., Devdariani, A. Z., & Golubkov, M. G. (2002). Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential. Journal of Experimental and Theoretical Physics, 95(6), 987-997. https://doi.org/10.1134/1.1537291

Vancouver

Golubkov GV, Devdariani AZ, Golubkov MG. Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential. Journal of Experimental and Theoretical Physics. 2002 Дек. 1;95(6):987-997. https://doi.org/10.1134/1.1537291

Author

Golubkov, G. V. ; Devdariani, A. Z. ; Golubkov, M. G. / Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential. в: Journal of Experimental and Theoretical Physics. 2002 ; Том 95, № 6. стр. 987-997.

BibTeX

@article{32c9dabe8c7f426e8e52285ef2d89594,
title = "Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential",
abstract = "A method for calculating the complex optical potential of slowly colliding Rydberg atom A** and neutral atom B in the ground electronic state is suggested. The method is based on the asymptotic approach and the theory of multichannel quantum defects, which uses the formalism of renormalized Lippmann-Schwinger equations. The potential is introduced as the 〈q|V opt|q〉 matrix element of the optical interaction operator, for which the integral equation is derived, and is calculated in the basis set of free particle wave functions |q〉. Fairly simple equations for the shift and broadening of the ionic term are obtained, and the principal characteristics of these equations are analyzed. By way of illustration, the optical potential of the Na**(nl) + B systems, where B is a rare gas atom, is calculated.",
keywords = "DIATOMIC-MOLECULES, EXCITED MOLECULES, SLOW COLLISIONS, PHOTOASSOCIATION, TRANSITIONS, ENERGY, GAS",
author = "Golubkov, {G. V.} and Devdariani, {A. Z.} and Golubkov, {M. G.}",
year = "2002",
month = dec,
day = "1",
doi = "10.1134/1.1537291",
language = "English",
volume = "95",
pages = "987--997",
journal = "Journal of Experimental and Theoretical Physics",
issn = "1063-7761",
publisher = "МАИК {"}Наука/Интерпериодика{"}",
number = "6",

}

RIS

TY - JOUR

T1 - Collision of Rydberg atom A** with atom B in the ground electronic state. Optical potential

AU - Golubkov, G. V.

AU - Devdariani, A. Z.

AU - Golubkov, M. G.

PY - 2002/12/1

Y1 - 2002/12/1

N2 - A method for calculating the complex optical potential of slowly colliding Rydberg atom A** and neutral atom B in the ground electronic state is suggested. The method is based on the asymptotic approach and the theory of multichannel quantum defects, which uses the formalism of renormalized Lippmann-Schwinger equations. The potential is introduced as the 〈q|V opt|q〉 matrix element of the optical interaction operator, for which the integral equation is derived, and is calculated in the basis set of free particle wave functions |q〉. Fairly simple equations for the shift and broadening of the ionic term are obtained, and the principal characteristics of these equations are analyzed. By way of illustration, the optical potential of the Na**(nl) + B systems, where B is a rare gas atom, is calculated.

AB - A method for calculating the complex optical potential of slowly colliding Rydberg atom A** and neutral atom B in the ground electronic state is suggested. The method is based on the asymptotic approach and the theory of multichannel quantum defects, which uses the formalism of renormalized Lippmann-Schwinger equations. The potential is introduced as the 〈q|V opt|q〉 matrix element of the optical interaction operator, for which the integral equation is derived, and is calculated in the basis set of free particle wave functions |q〉. Fairly simple equations for the shift and broadening of the ionic term are obtained, and the principal characteristics of these equations are analyzed. By way of illustration, the optical potential of the Na**(nl) + B systems, where B is a rare gas atom, is calculated.

KW - DIATOMIC-MOLECULES

KW - EXCITED MOLECULES

KW - SLOW COLLISIONS

KW - PHOTOASSOCIATION

KW - TRANSITIONS

KW - ENERGY

KW - GAS

UR - http://www.scopus.com/inward/record.url?scp=33748093382&partnerID=8YFLogxK

U2 - 10.1134/1.1537291

DO - 10.1134/1.1537291

M3 - Article

AN - SCOPUS:33748093382

VL - 95

SP - 987

EP - 997

JO - Journal of Experimental and Theoretical Physics

JF - Journal of Experimental and Theoretical Physics

SN - 1063-7761

IS - 6

ER -

ID: 28476209