dc.contributor.author |
Komninos, Y |
en |
dc.contributor.author |
Aspromallis, G |
en |
dc.contributor.author |
Nicolaides, CA |
en |
dc.date.accessioned |
2014-03-01T11:45:40Z |
|
dc.date.available |
2014-03-01T11:45:40Z |
|
dc.date.issued |
1996 |
en |
dc.identifier.issn |
0953-4075 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/37538 |
|
dc.subject.classification |
Optics |
en |
dc.subject.classification |
Physics, Atomic, Molecular & Chemical |
en |
dc.title |
The F-2(o) Rydberg series and low-lying autoionizing states of Al |
en |
heal.type |
other |
en |
heal.language |
English |
en |
heal.publicationDate |
1996 |
en |
heal.abstract |
By applying a theory which unifies the ab initio treatment of electronic structure, of electron correlation and of valence-Rydberg-continuum interactions, we calculated hitherto unknown properties of the Al F-2(o) spectrum. The KL(3s3p)P-3(o) nd states lie above threshold, starting with the 3d state at 3.0 eV. They decay by autoionization with rates of the order of 10(12) s(-1). The higher-lying autoionizing (3s3p)P-1(o) nd states exhibit a stronger interaction with the 3s(2)nf, epsilon f channel, resulting in an increase of the sr;all quantum defect of the Rydberg series from its Hartree-Fock value by a factor of 20. Using a correlated wavefunction for the D-2 lowest state, the oscillator strengths for D-2-F-2(o) transitions for low n, for high n and for free-electron energies up to 2.7 eV are computed. |
en |
heal.publisher |
IOP PUBLISHING LTD |
en |
heal.journalName |
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS |
en |
dc.identifier.isi |
ISI:A1996UD88000004 |
en |
dc.identifier.volume |
29 |
en |
dc.identifier.issue |
6 |
en |
dc.identifier.spage |
L193 |
en |
dc.identifier.epage |
L196 |
en |