1990
DOI: 10.1016/0301-0104(90)89079-6
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XC and HFD-B potential energy curves for Xe-Xe and related physical properties

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Cited by 136 publications
(100 citation statements)
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“…However, recent experiments on the commensurate ͑ ͱ 3 ϫ ͱ 3͒R30°Xe monolayers adsorbed on Cu͑111͒ 4 and Pt͑111͒ 5 surfaces have contradicted this simple picture in two important aspects: ͑i͒ the adsorption sites for Xe atoms deduced from the measurements were on top of the Cu 6 and Pt 7,8 atoms instead in the highly coordinated threefold hollow sites, and ͑ii͒ the frequencies of inplane vibrations in monolayer Xe/ Cu͑111͒ 9-11 as measured by He atom scattering ͑HAS͒ turned out lower than could have been expected from the force constants calculated for unconstrained Xe adlayers by using accurate pairwise atomic gas phase potentials. 12 Similar observations were made also for Xe adsorption on Cu͑100͒ 10 and Cu͑110͒ 13 surfaces. For the Xe/ Pt͑111͒ the absence of any significant dispersion of in-plane vibrations in the dilated commensurate Xe monolayer prevented unambiguous assignments of the measured dispersion curves.…”
Section: Introductionsupporting
confidence: 68%
“…However, recent experiments on the commensurate ͑ ͱ 3 ϫ ͱ 3͒R30°Xe monolayers adsorbed on Cu͑111͒ 4 and Pt͑111͒ 5 surfaces have contradicted this simple picture in two important aspects: ͑i͒ the adsorption sites for Xe atoms deduced from the measurements were on top of the Cu 6 and Pt 7,8 atoms instead in the highly coordinated threefold hollow sites, and ͑ii͒ the frequencies of inplane vibrations in monolayer Xe/ Cu͑111͒ 9-11 as measured by He atom scattering ͑HAS͒ turned out lower than could have been expected from the force constants calculated for unconstrained Xe adlayers by using accurate pairwise atomic gas phase potentials. 12 Similar observations were made also for Xe adsorption on Cu͑100͒ 10 and Cu͑110͒ 13 surfaces. For the Xe/ Pt͑111͒ the absence of any significant dispersion of in-plane vibrations in the dilated commensurate Xe monolayer prevented unambiguous assignments of the measured dispersion curves.…”
Section: Introductionsupporting
confidence: 68%
“…Considering that these structures have been observed in experiments for I-Pt͑111͒ and Xe-Pd͑111͒, we could use the data about magnitudes of adsorbate-substrate and adsorbate-adsorbate interactions to estimate the necessary conditions for the theory in this paper to be valid. The HFD-B2 model 32 augmented by McLachlan dispersion 37 has been frequently used for the description of lateral interactions of the rare-gas monolayers on metal surfaces. 31 The magnitude of lateral interactions for the XePd͑111͒ system should be similar to Xe-Pt͑111͒.…”
Section: Hexagonal Monolayers and Rigid Approximationmentioning
confidence: 99%
“…Xe-Pt͑111͒ and Xe-Pd͑111͒ are chosen as examples of rare-gas adsorption on metal surfaces, for which analytic expressions for adsorbate-adsorbate interactions are well known. 31,32 In order to see if the usual one-term Fourier expansion with V G 0 coefficient is a good approximation to the adsorbate-substrate interaction in these systems, the ͑E atop − E bridge ͒ / ͑E atop − E fcc ͒ ratio is used. This ratio for a one-term expansion should be around 0.89.…”
Section: Hexagonal Monolayers and Rigid Approximationmentioning
confidence: 99%
“…The normal modes of the monolayer solid are evaluated using the HFD-B2 Xe-Xe potential 32 supplemented by the McLachlan substratemediated dispersion energy. Some of the calculated phonon energies are listed in Table II.…”
Section: F Interactions and Scattering Conditionsmentioning
confidence: 99%