2015
DOI: 10.1103/physreva.92.052712
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Unified calculation of generalized oscillator strength of argon ranging from bound to continuum states

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Cited by 9 publications
(38 citation statements)
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“…From the geometric view, Eqs ( 4b ) and ( 5 ) can be represented as a one-dimension curve and a (N th − 1)-dimension surface in a N th dimensional space respectively. For cases with , which are somewhat different from the case associated with only two thresholds 19 21 , 25 – 28 , 35 , 36 , where the solutions of the Eqs ( 4b ) and ( 5 ) can be represented graphically in a plot with the only two effective principal quantum numbers. More specifically, with only two thresholds, there are two sets of effective principal quantum numbers, n 1 number of ν 1 corresponding to the first threshold I one and n 2 number of ν 2 corresponding to the second threshold I two with I one < I two .…”
Section: Resultsmentioning
confidence: 99%
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“…From the geometric view, Eqs ( 4b ) and ( 5 ) can be represented as a one-dimension curve and a (N th − 1)-dimension surface in a N th dimensional space respectively. For cases with , which are somewhat different from the case associated with only two thresholds 19 21 , 25 – 28 , 35 , 36 , where the solutions of the Eqs ( 4b ) and ( 5 ) can be represented graphically in a plot with the only two effective principal quantum numbers. More specifically, with only two thresholds, there are two sets of effective principal quantum numbers, n 1 number of ν 1 corresponding to the first threshold I one and n 2 number of ν 2 corresponding to the second threshold I two with I one < I two .…”
Section: Resultsmentioning
confidence: 99%
“…We return to examine photoionization processes of Ne + from both the and initial states. With the calculated MQDT parameters for all 1/2 + , 3/2 + , 5/2 + final channels, photoionization cross sections, i.e., the oscillator strength densities 21 for all eigenchannels are calculated. As shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…The relativistic eigenchannel R-matrix method (R-R-eigen) [8][9][10][11][12][13][14] is applied in this study to stringently treat the complex atomic multielectron problem. Briefly, the coupling of Nelectron ion-core target states and an excited electron with the appropriate angular momentum forms channels for the N + 1-electron excited complex with a specific total angular momentum.…”
Section: A Calculation Of Eigenchannel Parametersmentioning
confidence: 99%
“…Our R-R-eigen method [8][9][10][11][12][13][14] differs from the traditional R-matrix method [22][23][24][25][26][27] mainly by definitions of physical channels, which includes not only opened channels (with positive orbital energies) but also several relevant closed channels (with negative orbital energies). Therefore, physical channels (the number of which is denoted as n p ) include all Rydbergtype bound electrons and their adjacent continua with orbital energy in the energy range of ε > −q 2 /l 2 (in Ry, where q is the charge of a long-range potential and l is the orbital angular momentum of the electron) owing to the mathematical properties of Coulomb wave functions [20].…”
Section: A Calculation Of Eigenchannel Parametersmentioning
confidence: 99%
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