1981
DOI: 10.1143/jpsj.50.2643
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Optical Spectra of Hexagonal Ice

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Cited by 59 publications
(46 citation statements)
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“…Note that the relative absorbance of each spectrum has been normalized to account for the differences in density (concentration) when calculating the molar extinction coefficient, e. The room-temperature spectrum acquired at 23°C shows a peak at 8.46 eV with e ¼ 1,590 M À 1 cm À 1 . We note that the extinction coefficient confirms values from previous work 18 , however the peak energy is observed to be Comparison of absorption spectra from the literature showing the lowest-lying electronic transition in the vacuum ultraviolet for gas-phase (red line) 17 and liquid phase (black line) 18 water, and for water ice (blue line) 36 . Note the considerable blueshift in the condensed-phase spectra, attributed to extensive H-bond coordination lowering the ground-state energy, and introducing solvation, Rydbergization, Pauli repulsion and excitonic effects on the excited state.…”
Section: Resultssupporting
confidence: 87%
“…Note that the relative absorbance of each spectrum has been normalized to account for the differences in density (concentration) when calculating the molar extinction coefficient, e. The room-temperature spectrum acquired at 23°C shows a peak at 8.46 eV with e ¼ 1,590 M À 1 cm À 1 . We note that the extinction coefficient confirms values from previous work 18 , however the peak energy is observed to be Comparison of absorption spectra from the literature showing the lowest-lying electronic transition in the vacuum ultraviolet for gas-phase (red line) 17 and liquid phase (black line) 18 water, and for water ice (blue line) 36 . Note the considerable blueshift in the condensed-phase spectra, attributed to extensive H-bond coordination lowering the ground-state energy, and introducing solvation, Rydbergization, Pauli repulsion and excitonic effects on the excited state.…”
Section: Resultssupporting
confidence: 87%
“…The ubiquitous influence of long-ranged van der Waals interactions manipulates the melting behavior and, as described above, their detailed influence at the surface of ice is rather rich, often requiring a complete frequency-dependent treatment ͑Dzyaloshinskii et Ketcham and Hobbs, 1969;Daniels, 1971;Knight, 1971;Seki et al, 1981;Elbaum and Schick, 1991;Wilen et al, 1995;Benatov and Wettlaufer, 2004͒. Ostensibly the same physical phenomena underlie Derjaguin-Landau-Verwey-Overbeek ͑DLVO͒ theory, which assesses the competition between the screened Coulomb and attractive van der Waals interactions ͑Der-jaguin and Landau, 1941; Verwey and Overbeek, 1948͒.…”
Section: Impuritiesmentioning
confidence: 99%
“…In the photolysis of amorphous solid water ͑ASW͒ at the vacuum ultraviolet ͑vuv͒ region, the penetration depths are ϳ100 and ϳ35 nm for the first band at = 157 and 140 nm, respectively, and ϳ50 nm for the second band at = 122 nm. 9 Various photoproducts were detected in and on ice at 10 K. 10 The main photoproducts, OH, H 2 O 2 , and HO 2 , were the primary and secondary photoproducts of reaction ͑2͒. In the condensed phase photolysis, not only the primary unimolecular reactions but also the secondary reactions would be the sources of photoproducts.…”
Section: H 2 O + H → H + Oh ͑2͒mentioning
confidence: 99%