1997
DOI: 10.1088/0953-4075/30/19/017
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Angle-resolved Auger spectra of the molecule

Abstract: Auger decay spectra of the ethyne (acetylene) molecule have been measured at photon energies below as well as above the C 1s ionization threshold. Angular anisotropy has been observed at the π * resonance and in the region of a continuum feature previously assigned to a σ * resonance, but disappears far above threshold. Because of strong configuration interaction in the final state only high kinetic energy Auger transitions can be assigned to individual electronic states. In the case of resonant Auger decay, t… Show more

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Cited by 36 publications
(51 citation statements)
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“…The and symmetries are resolved completely in C 2 H 2 , as well as in N 2 and CO, except for the lowest absorption feature with a term value (T) of 2.8-3.4 eV. Some groups [93,94] assigned the 1s→ 3sσ g and 3pσ u Rydberg excited states to the lowest feature with T = 2.8-3.4 eV. However, both the 1s → 3pσ u and 3pπ u Rydberg transitions with T = 2.5 eV are clearly resolved as strong peaks, whereas the npσ Rydberg series is weak in N 2 and CO.…”
Section: Arpis Of C 2 Hmentioning
confidence: 91%
“…The and symmetries are resolved completely in C 2 H 2 , as well as in N 2 and CO, except for the lowest absorption feature with a term value (T) of 2.8-3.4 eV. Some groups [93,94] assigned the 1s→ 3sσ g and 3pσ u Rydberg excited states to the lowest feature with T = 2.8-3.4 eV. However, both the 1s → 3pσ u and 3pπ u Rydberg transitions with T = 2.5 eV are clearly resolved as strong peaks, whereas the npσ Rydberg series is weak in N 2 and CO.…”
Section: Arpis Of C 2 Hmentioning
confidence: 91%
“…The core-excited spectrum of C 2 H 2 is dominated by the C 1σ u −→ 1π g transition at 285.8 eV photon energy as seen in Fig. 30 (see [222]). The process under investigation is…”
Section: Two Examples: Angle-resolved Photoionization and Auger Spectmentioning
confidence: 92%
“…spectrum includes neither vibrational structures (not even resolved in the experimental spectrum by Kivimäki et al [222]), nor the broadening and profile deformation of the spectral lines due to vibrational transitions. Comparison with the experimental spectrum requires one to account for the characteristics of both the incident radiation, almost perfectly polarized alongẑ, but having a finite dispersion ( 0.6 eV in Kivimäki's experiment) around the exciting frequency and the finite energy resolution of the electron spectrometer: as by Eq.…”
Section: Two Examples: Angle-resolved Photoionization and Auger Spectmentioning
confidence: 94%
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