1994
DOI: 10.1016/0368-2048(93)02050-v
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Coherent excitation of vibrational wave functions observed in core hole decay spectra of O2, N2 and CO

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Cited by 178 publications
(112 citation statements)
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“…(4) coincides with conventional C1s → π * absorption spectroscopy [51]. The negative parts in the spectra around 287.2 eV mainly come from the emissions |ν = 1 R → |ν = 1 I .…”
Section: Numerical Resultssupporting
confidence: 81%
“…(4) coincides with conventional C1s → π * absorption spectroscopy [51]. The negative parts in the spectra around 287.2 eV mainly come from the emissions |ν = 1 R → |ν = 1 I .…”
Section: Numerical Resultssupporting
confidence: 81%
“…Although the valence electrons are delocalized in a condensed phase, the involvement of the core level makes both XRS and XES very local probes of the electronic structure (23). Furthermore, the attosecond time scale of the XRS excitation process and the O 1s life time of Ϸ4 fs in XES (24) are much shorter than the 1-2 ps typical for H-bond dynamics (25).…”
Section: Figurementioning
confidence: 99%
“…Since then, it was experimentally identified in several experiments like e.g. the first C1s → π * resonant Auger spectrum for CO, excited by narrow monochromator bandwidth synchrotron radiation, where it gave rise to modulations of the final state vibrational intensity distributions which could not be explained by a simple FranckCondon two-step excitation-deexcitation picture [16]. A more recent study of LVI can be found, for instance, in Ref.…”
Section: Interference Phenomenamentioning
confidence: 99%
“…[18] and references therein). Furthermore, the vibrational intensity distribution in the final state may vary strongly upon tuning of the excitation energy across the intermediate resonance state [16,19]. Fig.…”
Section: Interference Phenomenamentioning
confidence: 99%