Beam-foil spectroscopy of neon in the wavelength range 209–602 Å

Kernahan, J. A.; Donnelly, K. E.; Pinnington, E. H.

doi:10.1139/p77-167

Cited by 19 publications

(3 citation statements)

References 2 publications

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“…Apart from the resonance transition in oxygen, the available experimental data on the oxygen isoelectronic sequence are rather sparse. These few data are shown in table 4 [23][24]. For the 2p-3d transition in F +1 the computed value 0.1344 is within the error bounds of the experimental value 0.16 + 0.04.…”

Section: Methods Of Calculationsupporting

confidence: 61%

Optical oscillator strengths for the oxygen isoelectronic sequence

Ganas¹

1980

Molecular Physics

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An analytic atomic independent particle model potential adjusted to experimental single-particle energy levels is used to generate wavefunctions for the valence and excited states of 0, F +I, Ne +2, Na +3, Mg +4 and A1 +5. Using these wavefunctions in conjunction with the Born approximation and the LS-coupling scheme, we calculate optical oscillator strengths for excitations from the ls 2 2s 2 2p4(aP2) ground state. Good agreement is obtained with experimental data. Systematic trends along the isoelectronic sequence are discussed.

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Section: Methods Of Calculationsupporting

confidence: 61%

Optical oscillator strengths for the oxygen isoelectronic sequence

Ganas¹

1980

Molecular Physics

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“…The last-named configuration played an indirect role as a correlation configuration-no resonances converging on terms of this configuration were considered. However, it proved to be of crucial importance in the model's yielding a good oscillator strength for the important Kernahan et al (1977). Cited by Burke and Taylor (1975).…”

Section: Ne' Target-state Wauejiinctionsmentioning

confidence: 99%

Formation of LaSi_2-xLayers on Si by High-Current La Ion Implantation

Tang¹,

Cheng²,

Wang³

et al. 2003

Jpn. J. Appl. Phys.

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The shapes of three low-energy resonance features in the photoionisation of neutral neon are calculated along with the total cross section in the low-energy region. The lowest singly excited resonance is in particularly good agreement with experiment. The complex amplitudes in the vicinity of the lines are plotted and discussed as an aid to understanding aspects of these resonance features. The experimental absence of the ls22s22p43s4p line, in particular, seems to be the result of the two open-channel amplitudes' fluctuating out of phase so that the sum of the resulting partial cross sections is not measurably disturbed.

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“…Beam-foil analyses of the Ne V spectrum are covering different spectral regions: 80-35081 [14], 1050-2000 and 2000-6000A [l5, 161,379-914A [17], 209-602A [18] and, more recently, 1700-2400A [19]. NeV transitions quoted in Kelly's [7] compilation are based on the analyses of Refs [8, Physica Scripta 55 121 and [14] but the results of Lindeberg [13], of Irwin et al [17] and of Vach et al [19] have not been retained.…”

Section: Introductionmentioning

confidence: 99%