2001
DOI: 10.1209/epl/i2001-00132-1
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A lattice gas model of II-VI(001) semiconductor surfaces

Abstract: We introduce an anisotropic two-dimensional lattice gas model of metal terminated II-VI(001) semiconductor surfaces. Important properties of this class of materials are represented by effective NN and NNN interactions, which result in the competition of two vacancy structures on the surface. We demonstrate that the experimentally observed c(2×2)-(2×1) transition of the CdTe(001) surface can be understood as a phase transition in thermal equilibrium. The model is studied by means of transfer-matrix and Monte Ca… Show more

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Cited by 11 publications
(9 citation statements)
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“…Measuring energy in units of |ε d |, we set ε d = −1. A model, where the underlying crystal was assumed to be fixed, has been studied elsewhere [11]. If the energy difference between a perfect c(2 × 2) arrangement and a perfect (2 × 1) arrangement is small and positive (−2 < ε x ≤ −1.9), this model explains the c(2 × 2)-(2 × 1) reordering as an accompanying effect of an order-disorder transition in thermal equilibrium.…”
mentioning
confidence: 99%
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“…Measuring energy in units of |ε d |, we set ε d = −1. A model, where the underlying crystal was assumed to be fixed, has been studied elsewhere [11]. If the energy difference between a perfect c(2 × 2) arrangement and a perfect (2 × 1) arrangement is small and positive (−2 < ε x ≤ −1.9), this model explains the c(2 × 2)-(2 × 1) reordering as an accompanying effect of an order-disorder transition in thermal equilibrium.…”
mentioning
confidence: 99%
“…Comparing our solid-on-solid model with the two-dimensional anisotropic lattice gas, we calculate the equilibrium values of C d AA , C x AA in the planar lattice gas model at the value of θ A we measure for AB at a given temperature, which can be done using transfer matrix techniques [11]. Although the non-equilibrium conditions of sublimation enhance the dominance of C However, a simple mapping of the surface layer of the sublimating system on a 2D lattice gas in thermal equilibrium is not possible.…”
mentioning
confidence: 99%
“…Despite the fact that significant sublimation sets in even below 570K, the temperature driven re-ordering of the Cd-terminated surface has been discussed in terms of a phase transition in effective equilibrium. 5,8,10,11 Electron counting rules, 12 and density functional theory (DFT) calculations [13][14][15] show that the simultaneous occupation of nearest neighbor (NN) sites in the y-direction should be extremely unlikely within a terminating Cd layer. Such pairs of NN-Cd would lead to an unfavorable local concentration of positive charges.…”
Section: Properties Of the Materials Systemmentioning
confidence: 99%
“…In earlier investigations we employed two-dimensional lattice gas models of the CdTe(001) surface 10,11 for the investigation of the temperature and flux dependence of surface reconstructions. Chemical bonds and the influence of the underlying crystal were accounted for by effective pairwise anisotropic interactions.…”
Section: Introductionmentioning
confidence: 99%
“…Biehl et al introduced the anisotropic two‐dimensional lattice gas model for investigations of the metal‐terminated II–VI (001) semiconductor surfaces 17–20. This model reproduces many of the characteristic features of these materials.…”
Section: Introductionmentioning
confidence: 99%