1990
DOI: 10.1016/s0009-2614(90)87090-e
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On the electronic structure of liquid water: Conduction-band tail revealed by photoionization data

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Cited by 75 publications
(82 citation statements)
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“…Here, the experimental data from Hasted, 1972 reported that O-H bond length and the angle of H-O-H of free H2O molecule are 0.96 Å and 104.5° respectively [41]. Moreover, our calculation on the electronic structure of HOMO-LUMO gap is 8.1 eV, which is in the range of experimental values from 7.0 eV [42] to 8.9 eV [43]. Thus, we may conclude that our model of an H2O molecule represents the real experimental findings for both structural parameter and electronic structure, as well as the obtained geometrical structure of our surface model in Fig.…”
Section: Resultssupporting
confidence: 52%
“…Here, the experimental data from Hasted, 1972 reported that O-H bond length and the angle of H-O-H of free H2O molecule are 0.96 Å and 104.5° respectively [41]. Moreover, our calculation on the electronic structure of HOMO-LUMO gap is 8.1 eV, which is in the range of experimental values from 7.0 eV [42] to 8.9 eV [43]. Thus, we may conclude that our model of an H2O molecule represents the real experimental findings for both structural parameter and electronic structure, as well as the obtained geometrical structure of our surface model in Fig.…”
Section: Resultssupporting
confidence: 52%
“…The former barrier height (V = 3.42 eV) was estimated from the contact potential difference obtained by Kelvin force microscopy (Fig.4). The latter (V = 0.72 eV) barrier height was estimated from the bottom of the conduction band of liquid water [31]. In spite of the large difference in the barrier heights (2.7 eV), the two curves became almost identical when d > (3/4)r.…”
Section: Images Of Kelvin Probe Force Microscopymentioning
confidence: 99%
“…Nous avons rCcemment proposC une interpretation analogue pour la photoionisation de l'eau pure et des solutions aqueuses diluCes (63). I1 a ainsi Ct C not6 que les courbes exprimant la variation du rendement d'ionisation (4,) en fonction de 1'Cnergie (E,,) des photons incidents dans la region du seuil Ctaient exponentielles.…”
Section: B Dynamique Et Mkcanisme(s) De Solvatationunclassified
“…Celui-ci n'a cependant pas encore CtC dCterminC expkrimentalement sans Cquivoque (pour le cas de l'eau, voir figure 40). Notons enfin que d'aprks le schCma prCcCdemment dCcrit pour la photoionisation de l'eau pure et des solutions aqueuses diluees (63), les Clectrons photoCjectCs ne seraient pas initialement dans un Ctat quasi-libre, mais se localiseraient directement h partir d'Ctats excitoniques, de type Mott-Wannier, du liquide (74) : thermalisation e t piCgeage seraient alors des processus quasi-synchrones. Les insuffisances des calculs actuels de simulation pour interprCter quantitativement l'hydratation de I'Clectron nous paraissent provenir de diffkrentes causes, parfois dCjA mentionnCes.…”
Section: B Dynamique Et Mkcanisme(s) De Solvatationunclassified