Triangular lattice ramp model: Difference between revisions
Jump to navigation
Jump to search
m (Triangular lattice model moved to Triangular lattice ramp model) |
Carl McBride (talk | contribs) m (Added a mention of the 3 dimensional ramp model.) |
||
| Line 1: | Line 1: | ||
{{Stub-general}} | {{Stub-general}} | ||
The '''triangular lattice ramp 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. As such it can be seen as a two dimensional analogue of the [[ramp model]]. In the high [[temperature]] limit this model becomes the [[hard hexagon lattice model]]. | ||
==See also== | ==See also== | ||
*[[Building up a triangular lattice]] | *[[Building up a triangular lattice]] | ||
Revision as of 09:26, 22 July 2009
|
This article is a 'stub' page, it has no, or next to no, content. It is here at the moment to help form part of the structure of SklogWiki. If you add sufficient material to this article then please remove the {{Stub-general}} template from this page. |
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. As such it can be seen as a two dimensional analogue of the ramp model. In the high temperature limit this model becomes the hard hexagon lattice model.