EGAS41 - Swansea University
EGAS41 - Swansea University
EGAS41 - Swansea University
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41 st EGAS CP 22 Gdańsk 2009<br />
Two-electron-one-photon M1 and E2 transition between 2p 3 and<br />
2s 2 2p configuration of B-like ions<br />
J.G. Li 1,2 , C.Z. Dong 1,2,∗ , P. Jönsson 3 , G. Gaigalas 4,5<br />
1 College of Physics and Electronic Engineering, Northwest Normal <strong>University</strong>,<br />
Lanzhou 730070, China<br />
2 Joint Laboratory of Atomic Physics, NWNU & IMP CAS, Lanzhou 730070, China<br />
3 Nature, Environment, Society, Malmö <strong>University</strong>, Malmö S-20506, Sweden<br />
4 Department of Physics, Vilnius Pedagogical <strong>University</strong>, Studentu 39,<br />
Vilnius LT-08106, Lithuania<br />
5 Institute of Theoretical Physics and Astronomy, A. Goštauto 12, Vilnius LT-01108, Lithuania<br />
∗ Corresponding author: Dongcz@nwnu.edu.cn<br />
In the past years, there are many studies on energy structures, transition probabilities<br />
and relevant atomic properties of B-like ions. On the one hand, there exist strong configuration<br />
interactions between the 2s2p 2 configuration and the 2s 2 ns and 2s 2 nd Rydberg<br />
series. It is interesting to explore electron correlation, Breit interactions and quantum<br />
electrodynamical (QED) effects in the B-like ions [1,2]. On the other hand, B-like ions<br />
widely exist astrophysical [3] and laboratory plasma like EBIT or thermal nuclear fusion<br />
device [2,4]. Therefore, the transitions within the n = 2 complex including forbidden<br />
and resonance lines play key roles in diagnose of temperature, density and abundance of<br />
plasma [5].<br />
More recently, a large scale spectrum calculations on energy levels, specific mass shift<br />
parameters, hyperfine interaction constants, Landé g J factors and transition probabilities<br />
for C II, N III and O IV have been carried out by us [6] using GRASP2K package [7]<br />
based on multiconfiguration Dirac-Fock method. In this paper, we further calculated towelectron-one-photon<br />
(TEOP) M1 and E2 transitions between 2p 3 and 2s 2 2p configuration<br />
of B-like ions with 18 ≤ Z ≤ 74 [8]. The influence of Breit interaction and QED effect<br />
on concerned TEOP M1 and E2 transitions energies and probabilities were analyzed in<br />
detail. It was found that the contributions of Breit interaction to the TEOP transition<br />
can not be neglected especially for M1 decay.<br />
References<br />
[1] M.S. Safronova, W.R. Johnson, U.I. Safronova, Phys. Rev. A 54 2850 (1996)<br />
[2] E. Träbert, P. Beiersdorfer, J.K. Lepson, H. Chen, Phys. Rev. A 68 042501 (2003)<br />
[3] G.D. Sandlin, et al., Astron. Astrophys. Suppl. 61 801 (1986)<br />
[4] J.H. Davé, et al., J. Opt. Soc. Am. B 4 635 (1987)<br />
[5] B. Edlén, Phys. Scr. 28 483 1983<br />
[6] P. Jönsson, J.G. Li, G. Gaigalas, C.Z. Dong, Atomic Data Nuclear Data Table (in<br />
print) (2009)<br />
[7] P. Jönsson, X. He, Ch. Froese Fischer, I.P. Grant, Comput. Phys. Commun. 177<br />
(2007) 597<br />
[8] J.G. Li, C.Z. Dong, P. Jönsson, G. Gaigalas, Phys. Src. (to be submitted) (2009)<br />
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