EGAS41 - Swansea University
EGAS41 - Swansea University
EGAS41 - Swansea University
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41 st EGAS CP 23 Gdańsk 2009<br />
Hyperfine quenching of 3s3p 3 P 0 , 3 P 2 level of Mg-like ions<br />
H.H. Kang 1,2 , 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 />
Theoretical investigations on hyperfine quenching of metastable levels 3s3p 3 P 0 and 3 P 2<br />
of Mg-like ions between Z = 13 − 78 have been performed [1, 2] using Grasp2K package<br />
[3] based on the multi-configuration Dirac-Fock method. Electron correlation, Breit interaction<br />
and QED effects were taken into account systematically. Hyperfine quenching<br />
rates of 3s3p 3 P 0 level were compared with other theoretical [4, 5] and experimental values<br />
[6]. The present calculated probability of 4.327 × 10 −2 s −1 for 27 Al + is in good agreement<br />
with recent the experimental measurement of 4.854 × 10 −2 s −1 [6]. Furthermore, a fitting<br />
formula scaling in Z was obtained, which was presented in Fig.1 (a). In addition, it was<br />
found that the lifetime of 3s3p 3 P 2 level is sensitive to the hyperfine quenching at the<br />
beginning of the isoelectronic sequence as shown in Fig.1 (b).<br />
4.0<br />
3.2<br />
2.4<br />
1.6<br />
(a)<br />
10 7<br />
10 5<br />
HIT<br />
M1<br />
M2<br />
10 9 9/2<br />
(b)<br />
Log(A) (s -1 )<br />
0.8<br />
0.0<br />
-0.8<br />
-1.6<br />
-2.4<br />
A(I=1/2)<br />
A(I=5/2)<br />
A(I=3/2)<br />
A(I=7/2)<br />
Experimental value[6]<br />
A el<br />
A el = 1.087*10 -11 Z 7.8004<br />
Fitting by Brage[5]<br />
10 15 20 25 30 35 40 45 50 55 60 65 70 75 80<br />
Z<br />
log(A)(s -1 )<br />
10 3<br />
10 1<br />
10 -1<br />
10 -3<br />
7/2<br />
5/2<br />
3/2<br />
1/2<br />
10 -5<br />
10 15 20 25 30 35 40 45 50 55 60 65 70 75 80<br />
Z<br />
Figure 1: Logarithm of hyperfine induced transition rates A together with reduced hyperfine<br />
induced transition rates A el . (a): hyperfine quenching of 3 P 0 level, other theoretical and experimental<br />
results were shown; (b): hyperfine quenching 3 P 2 level compared with other main decay<br />
rates.<br />
References<br />
[1] H.H. Kang, J.G. Li, C.Z. Dong, P. Jönsson, G. Gaigalas, J. Phys. B (Submitted)<br />
(2009)<br />
[2] H.H. Kang, J.G. Li, C.Z. Dong, P. Jönsson, G. Gaigalas, (to be submitted) (2009)<br />
[3] P. Jönsson, X. He, Ch. Froese Fischer, I.P. Grant, Comput. Phys. Commun 177 597<br />
(2007)<br />
[4] J.P. Marques, F. Parente, P. Indelicato, At. Data Nucl. Data Tables 55 157 (1993)<br />
[5] T. Brage, et al., ApJ 500 507 (1996)<br />
[6] T. Rosenband, P.O. Schmidt, D.B. Hume, et al. Phys. Rev. Lett, 98, 220801 (2007)<br />
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