1995
DOI: 10.1016/0039-6028(94)00801-9
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Glancing-angle X-ray scattering studies of the premelting of ice surfaces

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Cited by 173 publications
(160 citation statements)
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“…In the vapor case, as N i increases, the film thickens, as expected, and the temperature at which this power law ͑d ϰ⌬T −1 ͒ begins to dominate the melting behavior decreases. The effect is particularly sensitive in the vapor case where it may overwhelm the incomplete melting controlled by van der Waals interactions in the pure case ͑Elbaum and Schick, 1991; and drive complete surface melting, thereby reconciling the difference between experimental observations made in different laboratories ͑Beaglehole and Nason, 1980; Dosch et al, 1996;Furukawa and Nada, 1997͒. As the temperature decreases, the first crossover to interfacial melting controlled by van der Waals interactions appears ͑d ϰ⌬T −1/3 ͒.…”
Section: Impuritiesmentioning
confidence: 71%
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“…In the vapor case, as N i increases, the film thickens, as expected, and the temperature at which this power law ͑d ϰ⌬T −1 ͒ begins to dominate the melting behavior decreases. The effect is particularly sensitive in the vapor case where it may overwhelm the incomplete melting controlled by van der Waals interactions in the pure case ͑Elbaum and Schick, 1991; and drive complete surface melting, thereby reconciling the difference between experimental observations made in different laboratories ͑Beaglehole and Nason, 1980; Dosch et al, 1996;Furukawa and Nada, 1997͒. As the temperature decreases, the first crossover to interfacial melting controlled by van der Waals interactions appears ͑d ϰ⌬T −1/3 ͒.…”
Section: Impuritiesmentioning
confidence: 71%
“…where q s is the surface charge density associated with the Bjerrum defect density ͑e.g., Dosch et al, 1996͒. In the classical context of DLVO theory, the Debye length is a constant, and Eq. ͑25͒ can be considered in the same sense as F vdW NR ͑d͒ above.…”
Section: Impuritiesmentioning
confidence: 99%
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“…, in greater density at crystal surfaces [Dosch et al, 1995[Dosch et al, , 1996, and even more at defects and rough surfaces [Mac and Higash, 1973]. On prismatic facets the equilibrium density of hydrogen bond disorder is PB = 5.7 x 10 25 m -3 averaged over a depth of 20 to 25 nm [Dosch et al, 1995[Dosch et al, , 1996.…”
Section: Bond Disorder and Ionization Exist In Bulk Icementioning
confidence: 99%
“…On prismatic facets the equilibrium density of hydrogen bond disorder is PB = 5.7 x 10 25 m -3 averaged over a depth of 20 to 25 nm [Dosch et al, 1995[Dosch et al, , 1996. The bond disorder implies a certain density of ionic defects: the ratio of ionic to bond defects is Pi / PB = 10 -5 in bulk ice near the melting point [Onsager and Dupuis, 1959].…”
Section: Bond Disorder and Ionization Exist In Bulk Icementioning
confidence: 99%