Fine structure and isotope shift of the 3s4d 3 D-3s3p 3 P, 3s5d 3 D-3s3p 3 P and 3p 2 3 P-3s3p 3 P Transitions of MgI
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Lifetimes of the 3 p 54 s 3 P 1 , 1 P 1 and 3 p 53 d 3 P 1 levels in K II
Oscillator strengths for the three lowest ground-state transitions 3p S0-3p 4s P1, 3p 6 S0-3p 4s P1, and 3p 6 S0-3p 3d P1 in argonlike K II are reported. The values were determined by lifetime measurements made using foil excitation of a fast ion beam, which yielded values t(4s P1)58.461.6 ns, t(3d P1)52.460.4 ns, and t(4s P1)50.4360.04 ns. Application of these results to the development of ext...
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A semiempirical method is used to characterize the 3s3p– 3s3p J=2 transition array in P II. In this method Slater, spin-orbit, and radial parameters are fitted to experimental energy levels to obtain a description of the array in terms of LS-coupling basis vectors. The intermediate coupling (IC) and configuration interaction (CI) amplitudes so obtained are then used to predict the branching fra...
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ژورنال
عنوان ژورنال: Il Nuovo Cimento D
سال: 1992
ISSN: 0392-6737
DOI: 10.1007/bf02451679