2005
DOI: 10.1103/physrevlett.95.133001
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Violation of the Franck-Condon Principle due to Recoil Effects in High Energy Molecular Core-Level Photoionization

Abstract: Carbon 1s photoelectron spectra of methane are measured over a photon energy range between 480 eV and 1200 eV. Additional components appear between the individual symmetric stretching vibrational components and are attributed to the excitations of asymmetric stretching and bending vibrations due to recoil of the high-energy photoelectron emission. This recoil effect is the evidence for the violation of the Franck-Condon principle which states that neither the positions nor the momenta of the nuclei change duri… Show more

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Cited by 135 publications
(83 citation statements)
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References 16 publications
(18 reference statements)
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“…40 A similar effect has been observed for CH 4 for the v = 1 and v = 2 components. 47 Figure 2 shows that vibrational excitations due to recoil effects are much less pronounced for BF 3 than for CF 4 (and CH 4 47 ). As can be seen, BF 3 photoionization leads to a large progression of vibrational levels in its symmetric stretching mode.…”
Section: Resultsmentioning
confidence: 99%
“…40 A similar effect has been observed for CH 4 for the v = 1 and v = 2 components. 47 Figure 2 shows that vibrational excitations due to recoil effects are much less pronounced for BF 3 than for CF 4 (and CH 4 47 ). As can be seen, BF 3 photoionization leads to a large progression of vibrational levels in its symmetric stretching mode.…”
Section: Resultsmentioning
confidence: 99%
“…This is partly due to the need for high kinetic-energy resolution in combination with high photon energy (that of x rays) but also to the fact that emission of a fast electron is accompanied by recoil of the residual cation [28], thus leading to a redistribution of the available energy even on symmetry-forbidden vibrational modes. As shown by Kukk et al [28], the recoil of CH + 4 ions leads to excitation of the asymmetric stretching and bending vibrations, which superimpose to the dominant symmetric stretching vibrational components. As a result, the apparent v ratios increase almost linearly with photon energy, thus hiding the underlying diffraction.…”
Section: Introductionmentioning
confidence: 99%
“…The specific example we consider here is vibrationally resolved C(1s) photoionization of CH 4 , a molecule for which there is a vast literature [26][27][28][29], but no evidence of diffraction has been reported so far. This is partly due to the need for high kinetic-energy resolution in combination with high photon energy (that of x rays) but also to the fact that emission of a fast electron is accompanied by recoil of the residual cation [28], thus leading to a redistribution of the available energy even on symmetry-forbidden vibrational modes.…”
Section: Introductionmentioning
confidence: 99%
“…For molecules, such recoil effects have been described for the first time in the pioneering work by Domcke and Cederbaum 9 . They are, however, rather weak in the soft X-ray regime up to about 1 keV in energy and have been observed only in recent years in photoelectron spectra: the first observation of vibrational recoil was observed by Kukk et al 10 in the methane molecule. Later on, this effect was more clearly observed in the tetrafluoro methane molecule CF 4 (ref.…”
mentioning
confidence: 99%