1998
DOI: 10.1103/physrevb.58.8704
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Monte Carlo simulation of a helium film on graphite

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Cited by 58 publications
(60 citation statements)
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“…Our results indicate that for large enough densities 6 (λ > 0.358Å −1 ) both the 1D and the tube arrangements have a localized (solid) phase and that the discontinuity in the density (if any) is surely very small. This is in agreement with the results discussed by Withlock et al [21] about the reduction of the size of this discontinuity from three to two dimensions: in 3D is fairly large, being considerably smaller in a purely 2D system. In 1D, we observe a further reduction towards a continuous or a quasi-continuous transition.…”
supporting
confidence: 82%
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“…Our results indicate that for large enough densities 6 (λ > 0.358Å −1 ) both the 1D and the tube arrangements have a localized (solid) phase and that the discontinuity in the density (if any) is surely very small. This is in agreement with the results discussed by Withlock et al [21] about the reduction of the size of this discontinuity from three to two dimensions: in 3D is fairly large, being considerably smaller in a purely 2D system. In 1D, we observe a further reduction towards a continuous or a quasi-continuous transition.…”
supporting
confidence: 82%
“…with Ψ c (R) = N i exp(−c r 2 i ) (r i being the radial distance of the particle to the center), that The binding energy of a single 4 He atom in graphite is E G B = 140.74 K [21], whereas in the nanotube we are studying is roughly three times larger, E T B = 429.97 K, a significant 4 difference that has been dramatically observed in the desorption experiment of Teizel et al [12]. On the other hand, the departure of the real 3D systems ( 4 He in graphite or a nanotube) from the idealized 2D or 1D liquids can be quantified by means of the parameter…”
mentioning
confidence: 99%
“…In fact, as it can be seen in Table 1, both energies are within each other error bars. However, for tubes whose radius is lower than the corresponding to a (10, 10) one, the lowest energy per particle correspond to an incommensurate solid (the (8,8) case is displayed as an example). On the other hand, the opposite happens for wider radii, of which the (12, 12) is chosen as a representative.…”
Section: Resultsmentioning
confidence: 99%
“…In the first studies of adsorption on graphite [8,12], a smoothed interaction that approached the C-He pair interaction sum was used. However, more recent studies [1,11,18] substitute this integrated potential by explicit pair sums that, in practice, can be tabulated in a grid for an efficient use in the simulation.…”
Section: Methodsmentioning
confidence: 99%
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