Electric-dipole oscillator strengths of 2p 63s 2 S e →2p 53s 2 2 P 0 transition in MgII, Al III and SiIV ions of the NaI isoelectronic sequence

1992 ◽  
Vol 14 (7) ◽  
pp. 739-743 ◽  
Author(s):  
S. N. Tiwary ◽  
D. D. Singh
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Isoelectronic Sequence ◽  
Dipole Oscillator

Electric Dipole Oscillator Strengths and Radiative Lifetimes in the Boron Isoelectronic Sequence

1987 ◽  
Vol 499 (6) ◽  
pp. 412-418 ◽  
Author(s):  
Th. M. El-Sherbini ◽  
A. A. Farrag ◽  
H. M. Mansour ◽  
A. A. Rahman
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Isoelectronic Sequence ◽  
Radiative Lifetimes ◽  
Dipole Oscillator

Systematic Trends in Atomic Oscillator Strengths: The Helium Isoelectronic Sequence

1972 ◽  
Vol 50 (12) ◽  
pp. 1363-1369 ◽  
Author(s):  
M. Cohen ◽  
R. P. McEachran
Keyword(s):  
Electric Dipole ◽  
Nuclear Charge ◽  
Principal Quantum Number ◽  
Wave Functions ◽  
Oscillator Strengths ◽  
Isoelectronic Sequence ◽  
Dipole Oscillator ◽  
Good Agreement ◽  
Comparison Data ◽  
Dipole Length

Electric dipole oscillator strengths (f values) have been calculated for a large number of singlet and triplet S–P, P–D, and D–F transitions in the helium isoelectronic sequence through O+6. The analytical orbital wave functions employed were of frozen-core type, and generally produce very good agreement between length and velocity values of the calculated oscillator strengths. A conspicuous exception occurs in many cases where the principal quantum number remains unchanged in the transition, and the more reliable dipole length values have been adopted for such transitions. The smooth variation of the calculated f values as functions of the inverse of the nuclear charge Z provided a sensitive check on the accuracy of the computations and indicated a considerable number of P–D transitions where the velocity values seemed the more reliable. Wherever comparison data are available, our calculated oscillator strengths are in excellent agreement with the most accurate values; in other cases, the absolute uncertainty in the f values should in no case exceed 5%.

Multichannel calculation of the electric-dipole oscillator strengths for the discrete 1Se1Po transitions in helium within the hyperspherical adiabatic approach

1991 ◽  
Vol 152 (9) ◽  
pp. 467-471 ◽  
Author(s):  
A.G. Abrashkevich ◽  
D.G. Abrashkevich ◽  
M.I. Gaysak ◽  
V.I. Lendyel ◽  
I.V. Puzynin ◽  
...  
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Adiabatic Approach ◽  
Dipole Oscillator ◽  
Hyperspherical Adiabatic

Electric Dipole Oscillator Strength and Radiative Lifetimes in the Magnesium Isoelectronic Sequence

1988 ◽  
Vol 500 (7) ◽  
pp. 498-506 ◽  
Author(s):  
Th. M. El-Sherbini ◽  
H. M. M. Mansour ◽  
A. A. Farag ◽  
A. A. Rahman
Keyword(s):  
Oscillator Strength ◽  
Electric Dipole ◽  
Isoelectronic Sequence ◽  
Radiative Lifetimes ◽  
Dipole Oscillator

Electric dipole oscillator strengths: length and velocity!

1983 ◽  
Vol 95 (6) ◽  
pp. 568-572 ◽  
Author(s):  
D.V.I. Roginsky ◽  
M. Klapisch ◽  
M. Cohen
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Dipole Oscillator

Two-electron-jump electric dipole oscillator strengths inLa48+andLa49+

1988 ◽  
Vol 38 (11) ◽  
pp. 5925-5927
Author(s):  
Donald R. Beck ◽  
George Aspromallis
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Dipole Oscillator
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