Triangular lattice ramp model: Difference between revisions
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The '''triangular lattice model''' | The '''triangular lattice ramp model''' | ||
<ref>[http://arxiv.org/abs/0907.3447 Noe G. Almarza, Jose A. Capitan, Jose A. Cuesta, Enrique Lomba "Phase diagram of a two-dimensional lattice gas model of a ramp system", arXiv:0907.3447v1 20 July (2009)]</ref> is a [[Idealised_models#Lattice_models| lattice model]] that consists of an exclusion of the six nearest neighbour sites of an occupied node, as well as a repulsion for next-nearest neighbours. In the high [[temperature]] limit this model becomes the [[hard hexagon lattice model]]. | <ref>[http://arxiv.org/abs/0907.3447 Noe G. Almarza, Jose A. Capitan, Jose A. Cuesta, Enrique Lomba "Phase diagram of a two-dimensional lattice gas model of a ramp system", arXiv:0907.3447v1 20 July (2009)]</ref> is a [[Idealised_models#Lattice_models| lattice model]] that consists of an exclusion of the six nearest neighbour sites of an occupied node, as well as a repulsion for next-nearest neighbours. In the high [[temperature]] limit this model becomes the [[hard hexagon lattice model]]. | ||
==See also== | ==See also== | ||
Revision as of 18:12, 21 July 2009
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The triangular lattice ramp model [1] is a lattice model that consists of an exclusion of the six nearest neighbour sites of an occupied node, as well as a repulsion for next-nearest neighbours. In the high temperature limit this model becomes the hard hexagon lattice model.