Triangular lattice ramp model: Difference between revisions
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The '''triangular lattice ramp model''' | The '''triangular lattice ramp model''' | ||
<ref> [http://dx.doi.org/10.1063/1.3223999 Noé G. Almarza, José A. Capitán, José A. Cuesta, and Enrique Lomba, "Phase diagram of a two-dimensional lattice gas model of a ramp system", Journal of Chemical Physics '''131''' 124506 (2009)] (see also [http://arxiv.org/abs/0907.3447 arXiv:0907.3447v1 20 July (2009)])</ref> is a [[Idealised_models#Lattice_models| lattice model]] | |||
<ref> [http://dx.doi.org/10.1063/1.3223999 Noé G. Almarza, José A. Capitán, José A. Cuesta, and Enrique Lomba, "Phase diagram of a two-dimensional lattice gas model of a ramp system", Journal of Chemical Physics '''131''' | |||
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]]. | 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== | ||
Latest revision as of 16:05, 28 September 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. 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.