1964
DOI: 10.1103/revmodphys.36.748
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The Solid State of Rare Gases

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Cited by 551 publications
(135 citation statements)
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“…As a result of comparison, differences between the interaction energies by the ab initio method and the pairwise-additive model were calculated to be The MC simulations were performed for XeBeO in solid Xe and Ar and for ArBeO in solid Ar under the periodic boundary condition (PBC) at temperature of T = 30 K. The fcc lattice was taken as a starting point for the initial configuration and 500 Xe (500 Ar) atoms were placed in a cubic box with a cell length of 30.6 Å (26.6 Å), which yields a density of 3.78 g/cm 3 (1.76 g/cm 3 ) and is close to the experimental value at the saturated vapor condition. 18 There are several possible sites at which Rg atom(s) can be substituted by RgBeO. As shown in Figure 4, one or two Rg atoms along the three possible orientations were replaced with a single RgBeO and these configurations were used to initiate MC simulations.…”
Section: A Ab Initio Calculations For Beo Xebeo and Arbeomentioning
confidence: 99%
“…As a result of comparison, differences between the interaction energies by the ab initio method and the pairwise-additive model were calculated to be The MC simulations were performed for XeBeO in solid Xe and Ar and for ArBeO in solid Ar under the periodic boundary condition (PBC) at temperature of T = 30 K. The fcc lattice was taken as a starting point for the initial configuration and 500 Xe (500 Ar) atoms were placed in a cubic box with a cell length of 30.6 Å (26.6 Å), which yields a density of 3.78 g/cm 3 (1.76 g/cm 3 ) and is close to the experimental value at the saturated vapor condition. 18 There are several possible sites at which Rg atom(s) can be substituted by RgBeO. As shown in Figure 4, one or two Rg atoms along the three possible orientations were replaced with a single RgBeO and these configurations were used to initiate MC simulations.…”
Section: A Ab Initio Calculations For Beo Xebeo and Arbeomentioning
confidence: 99%
“…3 we show the approach of the vibrational energy -23- Table Captions Table I: Parameter for Some Cases of Interest. A discussion of these parameters for the rare gas solids may be found in references [14] and [15]. For the case of…”
Section: Comparisonmentioning
confidence: 99%
“…When T/Gg is large the upper limit is small and the integrand can be ex panded to give dz=l (1-10) 0 z ^ or C\/ = 3Nkg, (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11) which is the Dulong and Petit Law. At very low temperatures Qp/T is large and may be taken to be infinity for all practical purposes.…”
Section: Debye Modelmentioning
confidence: 99%
“…At very low temperatures Qp/T is large and may be taken to be infinity for all practical purposes. The integral then is 4 % /15 from standard tables and S = "kg (^) , (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12) 3 which is the famous Debye T -law of specific heats.…”
Section: Debye Modelmentioning
confidence: 99%
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