IOP PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS
J. Phys. B: At. Mol. Opt. Phys. 46 (2013) 145002 (6pp) doi:10.1088/0953-4075/46/14/145002
Auger energies, branching ratios, widths
and x-ray rates of double K -vacancy states
of Ne
2+
: a close-coupling calculation
Yanpeng Liu, Jiaolong Zeng and Jianmin Yuan
Department of Physics, College of Science, National University of Defense Technology,
410073 Changsha Hunan, People’s Republic of China
E-mail: jiaolongzeng@hotmail.com
Received 1 May 2013, in final form 6 June 2013
Published 27 June 2013
Online at stacks.iop.org/JPhysB/46/145002
Abstract
A close-coupling calculation is performed for the photoionization cross section of the
high-lying core-excited state 1s2s
2
2p
51
P
o
of Ne
2+
in the energy region of the double
K-vacancy resonance 1s
0
2s
2
2p
61
S. The calculation is carried out by using the R-matrix
method in the LS-coupling scheme, which includes 27 target states and extensive configuration
interaction. The KK−KL x-ray energy, rate and autoionization width of the double K-vacancy
state, together with KK−KLL Auger energies and branching ratios of the main channels, are
obtained from the cross sections and the contributions of these channels. The calculated
resonance energy and x-ray rate are in good agreement with the existing experimental and
theoretical results. For the Auger width, our result agrees well with the available experimental
result and it is very close to the average of other theoretical data, which shows considerable
differences with each other. The Auger energy of the predominate channel KK−KL
23
L
23
2
D is
in rather good agreement with recent experiments on the Auger spectra. Our branching ratios
for the channels KK−KL
23
L
23
2
D and KK−KL
23
L
23
2
S are larger than the results obtained by
the multi-configuration Dirac–Fock method by ∼20% on average, which may be due to the
coupling of the continuum channels.
1. Introduction
The characteristics of the double K-vacancy states, known
as hollow atoms, have always attracted attention. The newly
arisen x-ray free-electron lasers (XFELs) providing very
intense femtosecond x-ray pulses were used to investigate
the atomic inner-shell processes [1–4]. The production of
the hollow states with an XFEL such as the linac coherent
light source is accessible since the sequential single-photon
absorption became the dominant mechanism [3]. This is quite
different from the energetic electrons’ impact [5, 6] and the
double photoionization of the K-shell by absorbing a single
photon of the x-ray synchrotron radiation [7, 8]. For low-
Z atoms such as neon, the double K-vacancy states mainly
decay by Auger transitions and can be observed by recording
KK−KLL Auger electron spectra [3, 5–7]. So the Auger
properties including energies, widths and branching ratios
are important in modelling the interaction of intense x-ray
lasers with atoms, molecules and clusters [9] and in modelling
the radiative properties of local thermodynamic equilibrium
(LTE) and non-LTE plasmas [10–14]. In addition, Auger
rates and branching ratios also play an important role in the
investigations of the double Auger decay and the cascade decay
from inner-shell vacancy states [15–18].
The Auger transitions of an autoionizing state are entirely
due to the electron–electron interactions, and strictly correlated
with the coupling of the discrete state and the continuum
channels. The close-coupling approximation was used to
obtain the properties of the single K-vacancy resonances for
atoms and ions such as B I [19], O I [20], Ne I [21], Al VII
[22], Ne VII [23], Fe XV [24] and the double K-vacancy
resonances for atomic lithium which has three electrons
[25–27]. To our knowledge, few close-coupling calculations
were reported for more complex systems with more than three
electrons such as 1s
0
2s
2
2p
6 1
S of Ne
2+
. Some theoretical
results were obtained by employing the multi-configuration
Dirac–Fock (MCDF) method [6, 28, 29] in the Hartree–Fock
(HF) model [30, 31], and some results were obtained in
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