| Autor: |
Zimbitas, G., Haq, S., Hodgson, A. |
| Předmět: |
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| Zdroj: |
Journal of Chemical Physics; 11/1/2005, Vol. 123 Issue 17, p174701, 9p, 2 Black and White Photographs, 5 Graphs |
| Abstrakt: |
When water is adsorbed on Pt(111) above 135 K several different ice structures crystallize, depending on the thickness of the ice layer. At low coverage water forms extended islands of ice with a ([Square_Root]37×[Square_Root]37)R25° unit cell, which compresses as the monolayer saturates to form a ([Square_Root]39×[Square_Root]39)R16° structure. The [Square_Root]39 low-energy electron diffraction (LEED) pattern becomes more intense as the second layer grows, remaining bright for films up of 10–15 layers and then fading and disappearing for films more than ca. 40 layers thick. The ice multilayer consists of an ordered [Square_Root]39 wetting layer, on which ice grows as a crystalline film which progressively loses its registry to the wetting layer. Ice films more than ca. 50 layers thick develop a hexagonal LEED pattern, the entire film and wetting layer reorienting to form an incommensurate bulk ice. These changes are reflected in the vibrational spectra which show changes in line shape and intensity associated with the different ice structures. Thin amorphous solid water films crystallize to form the same phases observed during growth, implying that these structures are thermodynamically stable and not kinetic phases formed during growth. The change from a [Square_Root]39 registry to incommensurate bulk ice at ca. 50 layers is associated with a change in crystallization kinetics from nucleation at the Pt(111) interface in thin films to nucleation of incommensurate bulk ice in amorphous solid water films more than 50 layers thick. [ABSTRACT FROM AUTHOR] |
| Databáze: |
Complementary Index |
| Externí odkaz: |
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