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Phys. Rev. A 76, 052501 (2007) [7 pages]

Zeeman splitting and g factor of the 1s22s22p 2P3∕2 and 2P1∕2 levels in Ar13+

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R. Soria Orts1, J. R. Crespo López-Urrutia1, H. Bruhns1, A. J. González Martínez1, Z. Harman1, U. D. Jentschura1, C. H. Keitel1, A. Lapierre1, H. Tawara1, I. I. Tupitsyn1,2, J. Ullrich1, and A. V. Volotka2
1Max Planck Institute for Nuclear Physics, Saupfercheckweg 1, D 69117 Heidelberg, Germany
2Department of Physics, St. Petersburg State University, Oulianovskaya 1, Petrodvorets, 198504 St. Petersburg, Russia

Received 27 March 2007; published 5 November 2007

The Zeeman line components of the magnetic-dipole (M1) 1s22s22p 2P1∕22P3∕2 transition in boronlike Ar13+ were experimentally resolved by high-precision emission spectroscopy using the Heidelberg electron beam ion trap. We determined the gyromagnetic (g) factors of the ground and first-excited levels to be g1∕2=0.663(7) and g3∕2=1.333(2), respectively. This corresponds to a measurement of the g factor of a relativistic electron in a bound non-S state of a multielectron ion with a 1.5 parts-per-thousand accuracy. The results are compared to theoretical calculations by means of the configuration interaction Dirac-Fock-Sturmian method including electron correlation effects and additional quantum electrodynamic corrections. Our measurements show that the classical Landé g factor formula is sufficiently accurate to the present level of accuracy in few-electron ions of medium nuclear charge number Z.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.76.052501
DOI:
10.1103/PhysRevA.76.052501
PACS:
31.30.Jv, 32.60.+i