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Renewed analysis of the hyperfine structure of the Na 2 1 3 Δ g state. / Sovkov, Vladimir B.; Xie, Feng; Li, Dan; Lukashov, Sergey S.; Baturo, Vera V.; Ma, Jie; LI, LI.

в: AIP Advances, Том 8, № 12, 125322, 01.12.2018.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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Sovkov, Vladimir B. ; Xie, Feng ; Li, Dan ; Lukashov, Sergey S. ; Baturo, Vera V. ; Ma, Jie ; LI, LI. / Renewed analysis of the hyperfine structure of the Na 2 1 3 Δ g state. в: AIP Advances. 2018 ; Том 8, № 12.

BibTeX

@article{51d446f4119c49ee914c207078874d3e,
title = "Renewed analysis of the hyperfine structure of the Na 2 1 3 Δ g state",
abstract = "The hyperfine structure on the levels of the Na 2 1 3Δ g state reported in Liu et al. [J. Chem. Phys. 115, 3647 (2001)] is analyzed using a new approach that overcomes most of the approximations adopted in the cited article. We exclude an approximation of the united atom, implying that the electron cloud only interacts with the total nuclear spin, and replace it with the interactions between individual nuclei and electrons. Rather than equating the observed intensities in the spectra with the populations of the hyperfine (HF) components of a 1 3Δ g state level excited from a hypothetical equilibrium HF ensemble in a state b 3Π 1u, we consider the more realistic excitation-de-excitation schemes in their entirety, and take into account the mixed character of the window levels of the A1Σu+∼b3ΠΩu system, which generally contains fractions of all Ω = 0, 1, 2. We also avoid an approximation of the major component, in which the probabilities of the optical dipole transitions are computed from the 0-th order state vector alone, and compute the contributions from all components of the blended states. The underlying theory and algorithms are described, and the parameters of the new model are fitted and reported. ",
keywords = "димер натрия, сверхтонкая структура, PFOODR",
author = "Sovkov, {Vladimir B.} and Feng Xie and Dan Li and Lukashov, {Sergey S.} and Baturo, {Vera V.} and Jie Ma and LI LI",
year = "2018",
month = dec,
day = "1",
doi = "10.1063/1.5055675",
language = "English",
volume = "8",
journal = "AIP Advances",
issn = "2158-3226",
publisher = "American Institute of Physics",
number = "12",

}

RIS

TY - JOUR

T1 - Renewed analysis of the hyperfine structure of the Na 2 1 3 Δ g state

AU - Sovkov, Vladimir B.

AU - Xie, Feng

AU - Li, Dan

AU - Lukashov, Sergey S.

AU - Baturo, Vera V.

AU - Ma, Jie

AU - LI, LI

PY - 2018/12/1

Y1 - 2018/12/1

N2 - The hyperfine structure on the levels of the Na 2 1 3Δ g state reported in Liu et al. [J. Chem. Phys. 115, 3647 (2001)] is analyzed using a new approach that overcomes most of the approximations adopted in the cited article. We exclude an approximation of the united atom, implying that the electron cloud only interacts with the total nuclear spin, and replace it with the interactions between individual nuclei and electrons. Rather than equating the observed intensities in the spectra with the populations of the hyperfine (HF) components of a 1 3Δ g state level excited from a hypothetical equilibrium HF ensemble in a state b 3Π 1u, we consider the more realistic excitation-de-excitation schemes in their entirety, and take into account the mixed character of the window levels of the A1Σu+∼b3ΠΩu system, which generally contains fractions of all Ω = 0, 1, 2. We also avoid an approximation of the major component, in which the probabilities of the optical dipole transitions are computed from the 0-th order state vector alone, and compute the contributions from all components of the blended states. The underlying theory and algorithms are described, and the parameters of the new model are fitted and reported.

AB - The hyperfine structure on the levels of the Na 2 1 3Δ g state reported in Liu et al. [J. Chem. Phys. 115, 3647 (2001)] is analyzed using a new approach that overcomes most of the approximations adopted in the cited article. We exclude an approximation of the united atom, implying that the electron cloud only interacts with the total nuclear spin, and replace it with the interactions between individual nuclei and electrons. Rather than equating the observed intensities in the spectra with the populations of the hyperfine (HF) components of a 1 3Δ g state level excited from a hypothetical equilibrium HF ensemble in a state b 3Π 1u, we consider the more realistic excitation-de-excitation schemes in their entirety, and take into account the mixed character of the window levels of the A1Σu+∼b3ΠΩu system, which generally contains fractions of all Ω = 0, 1, 2. We also avoid an approximation of the major component, in which the probabilities of the optical dipole transitions are computed from the 0-th order state vector alone, and compute the contributions from all components of the blended states. The underlying theory and algorithms are described, and the parameters of the new model are fitted and reported.

KW - димер натрия

KW - сверхтонкая структура

KW - PFOODR

UR - http://www.scopus.com/inward/record.url?scp=85058797038&partnerID=8YFLogxK

U2 - 10.1063/1.5055675

DO - 10.1063/1.5055675

M3 - Article

VL - 8

JO - AIP Advances

JF - AIP Advances

SN - 2158-3226

IS - 12

M1 - 125322

ER -

ID: 36732656