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@article{0a9114af74834c70b038243e92099fa7,
title = "Determination of the 2s22p5-2s2p6 transition energy in fluorine-like nickel utilizing a low-lying dielectronic resonance",
abstract = "High-precision spectroscopy of the low-lying dielectronic resonances in fluorine-like Ni19+ ions was studied by employing the electron-ion merged-beams method at the heavy-ion storage ring CSRm. The measured dielectronic-recombination (DR) resonances are identified by comparison with relativistic calculations utilizing the flexible atomic code. The lowest-energy resonance at about 86 meV is due to DR via the (2s2p6[2S1/2]6s)J=1 intermediate state. The position of this resonance could be determined within an experimental uncertainty of as low as ±4meV. The binding energy of the 6s Rydberg electron in the resonance state was calculated using two different approaches, the multiconfigurational Dirac-Hartree-Fock (MCDHF) method and the stabilization method (SM). The sum of the experimental (2s2p6[2S1/2]6s)J=1 resonance energy and the theoretical 6s binding energies from the MCDHF and SM calculations yields the following values for the 2s22p52P3/2→2s2p62S1/2 transition energy: 149.056(4)exp(20)theo and 149.032(4)exp(6)theo, respectively. The theoretical calculations reveal that second-order QED and third-order correlation effects contribute together about 0.1 eV to the total transition energy. The present precision DR spectroscopic measurement builds a bridge which enables comparisons between different theories. ",
author = "Wang, {S. X.} and Huang, {Z. K.} and Wen, {W. Q.} and Ma, {W. L.} and Wang, {H. B.} and S. Schippers and Wu, {Z. W.} and Kozhedub, {Y. S.} and Kaygorodov, {M. Y.} and Volotka, {A. V.} and K. Wang and Zhang, {C. Y.} and Chen, {C. Y.} and C. Liu and Huang, {H. K.} and L. Shao and Mao, {L. J.} and X. Ma and J. Li and Tang, {M. T.} and Yan, {K. M.} and Zhou, {Y. B.} and Yuan, {Y. J.} and Yang, {J. C.} and Zhang, {S. F.} and X. Ma and Zhu, {L. F.}",
note = "Publisher Copyright: {\textcopyright} 2022 American Physical Society. ",
year = "2022",
month = oct,
doi = "10.1103/PhysRevA.106.042808",
language = "English",
volume = "106",
journal = "Physical Review A - Atomic, Molecular, and Optical Physics",
issn = "1050-2947",
publisher = "American Physical Society",
number = "4",

}

RIS

TY - JOUR

T1 - Determination of the 2s22p5-2s2p6 transition energy in fluorine-like nickel utilizing a low-lying dielectronic resonance

AU - Wang, S. X.

AU - Huang, Z. K.

AU - Wen, W. Q.

AU - Ma, W. L.

AU - Wang, H. B.

AU - Schippers, S.

AU - Wu, Z. W.

AU - Kozhedub, Y. S.

AU - Kaygorodov, M. Y.

AU - Volotka, A. V.

AU - Wang, K.

AU - Zhang, C. Y.

AU - Chen, C. Y.

AU - Liu, C.

AU - Huang, H. K.

AU - Shao, L.

AU - Mao, L. J.

AU - Ma, X.

AU - Li, J.

AU - Tang, M. T.

AU - Yan, K. M.

AU - Zhou, Y. B.

AU - Yuan, Y. J.

AU - Yang, J. C.

AU - Zhang, S. F.

AU - Ma, X.

AU - Zhu, L. F.

N1 - Publisher Copyright: © 2022 American Physical Society.

PY - 2022/10

Y1 - 2022/10

N2 - High-precision spectroscopy of the low-lying dielectronic resonances in fluorine-like Ni19+ ions was studied by employing the electron-ion merged-beams method at the heavy-ion storage ring CSRm. The measured dielectronic-recombination (DR) resonances are identified by comparison with relativistic calculations utilizing the flexible atomic code. The lowest-energy resonance at about 86 meV is due to DR via the (2s2p6[2S1/2]6s)J=1 intermediate state. The position of this resonance could be determined within an experimental uncertainty of as low as ±4meV. The binding energy of the 6s Rydberg electron in the resonance state was calculated using two different approaches, the multiconfigurational Dirac-Hartree-Fock (MCDHF) method and the stabilization method (SM). The sum of the experimental (2s2p6[2S1/2]6s)J=1 resonance energy and the theoretical 6s binding energies from the MCDHF and SM calculations yields the following values for the 2s22p52P3/2→2s2p62S1/2 transition energy: 149.056(4)exp(20)theo and 149.032(4)exp(6)theo, respectively. The theoretical calculations reveal that second-order QED and third-order correlation effects contribute together about 0.1 eV to the total transition energy. The present precision DR spectroscopic measurement builds a bridge which enables comparisons between different theories.

AB - High-precision spectroscopy of the low-lying dielectronic resonances in fluorine-like Ni19+ ions was studied by employing the electron-ion merged-beams method at the heavy-ion storage ring CSRm. The measured dielectronic-recombination (DR) resonances are identified by comparison with relativistic calculations utilizing the flexible atomic code. The lowest-energy resonance at about 86 meV is due to DR via the (2s2p6[2S1/2]6s)J=1 intermediate state. The position of this resonance could be determined within an experimental uncertainty of as low as ±4meV. The binding energy of the 6s Rydberg electron in the resonance state was calculated using two different approaches, the multiconfigurational Dirac-Hartree-Fock (MCDHF) method and the stabilization method (SM). The sum of the experimental (2s2p6[2S1/2]6s)J=1 resonance energy and the theoretical 6s binding energies from the MCDHF and SM calculations yields the following values for the 2s22p52P3/2→2s2p62S1/2 transition energy: 149.056(4)exp(20)theo and 149.032(4)exp(6)theo, respectively. The theoretical calculations reveal that second-order QED and third-order correlation effects contribute together about 0.1 eV to the total transition energy. The present precision DR spectroscopic measurement builds a bridge which enables comparisons between different theories.

UR - http://www.scopus.com/inward/record.url?scp=85140245453&partnerID=8YFLogxK

UR - http://arxiv.org/abs/2205.01334

UR - https://www.mendeley.com/catalogue/ea3b3f30-104f-3a0d-9ada-179f66881697/

U2 - 10.1103/PhysRevA.106.042808

DO - 10.1103/PhysRevA.106.042808

M3 - Article

AN - SCOPUS:85140245453

VL - 106

JO - Physical Review A - Atomic, Molecular, and Optical Physics

JF - Physical Review A - Atomic, Molecular, and Optical Physics

SN - 1050-2947

IS - 4

M1 - 042808

ER -

ID: 99935778