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Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules. / Golovin, A. V.; Adachi, J.; Motoki, S.; Takahashi, M.; Yagishita, A.

в: Journal of Physics B: Atomic, Molecular and Optical Physics, Том 38, № 3, 01.02.2005, стр. L63-68.

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

Harvard

Golovin, AV, Adachi, J, Motoki, S, Takahashi, M & Yagishita, A 2005, 'Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules', Journal of Physics B: Atomic, Molecular and Optical Physics, Том. 38, № 3, стр. L63-68. https://doi.org/10.1088/0953-4075/38/3/L03

APA

Golovin, A. V., Adachi, J., Motoki, S., Takahashi, M., & Yagishita, A. (2005). Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules. Journal of Physics B: Atomic, Molecular and Optical Physics, 38(3), L63-68. https://doi.org/10.1088/0953-4075/38/3/L03

Vancouver

Golovin AV, Adachi J, Motoki S, Takahashi M, Yagishita A. Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules. Journal of Physics B: Atomic, Molecular and Optical Physics. 2005 Февр. 1;38(3):L63-68. https://doi.org/10.1088/0953-4075/38/3/L03

Author

Golovin, A. V. ; Adachi, J. ; Motoki, S. ; Takahashi, M. ; Yagishita, A. / Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules. в: Journal of Physics B: Atomic, Molecular and Optical Physics. 2005 ; Том 38, № 3. стр. L63-68.

BibTeX

@article{ce0fa30177a442ac8f062a2808021cd1,
title = "Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules",
abstract = "The photoelectron angular distributions (PADs) for the OCS O 1s, C 1s and S 2p1/2, 2p3/2 ionization have been measured in the shape resonance region. The experimental results have been compared with multiple scattering Xα calculations. It is found that the position of an ionized atom plays a significant role. For a central position (C Is ionization) the PAD is relatively symmetric. In the case of S 2p and O 1s ionization, electrons are emitted highly preferentially in a solid cone directed from the molecular centre to the respective S or O atom. For the OCS O Is ionization the S-C fragment plays a very effective role as a 'scatterer' and in the shape resonance region nearly all intensity in PAD is concentrated in the lobe between θ = 50° and 80°, but not along the molecular axis.",
author = "Golovin, {A. V.} and J. Adachi and S. Motoki and M. Takahashi and A. Yagishita",
year = "2005",
month = feb,
day = "1",
doi = "10.1088/0953-4075/38/3/L03",
language = "English",
volume = "38",
pages = "L63--68",
journal = "Quantum Optics",
issn = "0953-4075",
publisher = "IOP Publishing Ltd.",
number = "3",

}

RIS

TY - JOUR

T1 - Inner-shell photoelectron angular distributions from fixed-in-space OCS molecules

AU - Golovin, A. V.

AU - Adachi, J.

AU - Motoki, S.

AU - Takahashi, M.

AU - Yagishita, A.

PY - 2005/2/1

Y1 - 2005/2/1

N2 - The photoelectron angular distributions (PADs) for the OCS O 1s, C 1s and S 2p1/2, 2p3/2 ionization have been measured in the shape resonance region. The experimental results have been compared with multiple scattering Xα calculations. It is found that the position of an ionized atom plays a significant role. For a central position (C Is ionization) the PAD is relatively symmetric. In the case of S 2p and O 1s ionization, electrons are emitted highly preferentially in a solid cone directed from the molecular centre to the respective S or O atom. For the OCS O Is ionization the S-C fragment plays a very effective role as a 'scatterer' and in the shape resonance region nearly all intensity in PAD is concentrated in the lobe between θ = 50° and 80°, but not along the molecular axis.

AB - The photoelectron angular distributions (PADs) for the OCS O 1s, C 1s and S 2p1/2, 2p3/2 ionization have been measured in the shape resonance region. The experimental results have been compared with multiple scattering Xα calculations. It is found that the position of an ionized atom plays a significant role. For a central position (C Is ionization) the PAD is relatively symmetric. In the case of S 2p and O 1s ionization, electrons are emitted highly preferentially in a solid cone directed from the molecular centre to the respective S or O atom. For the OCS O Is ionization the S-C fragment plays a very effective role as a 'scatterer' and in the shape resonance region nearly all intensity in PAD is concentrated in the lobe between θ = 50° and 80°, but not along the molecular axis.

UR - http://www.scopus.com/inward/record.url?scp=24144483069&partnerID=8YFLogxK

U2 - 10.1088/0953-4075/38/3/L03

DO - 10.1088/0953-4075/38/3/L03

M3 - Article

VL - 38

SP - L63-68

JO - Quantum Optics

JF - Quantum Optics

SN - 0953-4075

IS - 3

ER -

ID: 5287954