Lattice hard spheres: Difference between revisions

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of sites separated by less than some short distance <math>  \sigma </math> cannot be simultaneously occupied.
of sites separated by less than some short distance <math>  \sigma </math> cannot be simultaneously occupied.


== Brief description of the models ==
Basically the differences with the standard [[Lattice gas|lattice gas]] model ([[Ising Models|Ising model]]) are:
Basically the differences with the standard [[Lattice gas|lattice gas]] model ([[Ising Models|Ising model]]) are:
   
   
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These systems exhibit phase (order-disorder) transitions  
These systems exhibit phase (order-disorder) transitions  
== Three-dimensional lattices ==
*See Ref. 1 for some results of three-dimensional lattice hard sphere systems (on a [[Building up a simple cubic lattice |simple cubic lattice]])


*See Ref. 1 for some results of three-dimensional lattice hard sphere systems (on a [[Building up a simple cubic lattice |simple cubic lattice]])
== Two-dimensional lattices ==


=== Square lattice  ===
*See Ref 2. for results of two-dimensional systems (lattice hard disks) on a square lattice.
*See Ref 2. for results of two-dimensional systems (lattice hard disks) on a square lattice.


The [[hard hexagon lattice model|hard hexagon lattice model]] belongs to this kind of models
=== Triangular lattice ===
The [[hard hexagon lattice model|hard hexagon lattice model]] belongs to this kind of models. In this model an occupied site
excluded the occupation of nearest neighbour positions. This model exhibits a continous transition. (See references
in the entry: [[hard hexagon lattice model|hard hexagon lattice model]]
 


== References ==
== References ==

Revision as of 12:53, 14 August 2008

Lattice hard spheres refers to athermal lattice gas models, in which pairs of sites separated by less than some short distance cannot be simultaneously occupied.

Brief description of the models

Basically the differences with the standard lattice gas model (Ising model) are:

  • An occupied site excludes the occupation of some of the neighboring sites.
  • No energy interactions between pairs of occupied sites are considered.

These systems exhibit phase (order-disorder) transitions

Three-dimensional lattices

  • See Ref. 1 for some results of three-dimensional lattice hard sphere systems (on a simple cubic lattice)

Two-dimensional lattices

Square lattice

  • See Ref 2. for results of two-dimensional systems (lattice hard disks) on a square lattice.

Triangular lattice

The hard hexagon lattice model belongs to this kind of models. In this model an occupied site excluded the occupation of nearest neighbour positions. This model exhibits a continous transition. (See references in the entry: hard hexagon lattice model


References

  1. A. Z. Panagiotopoulos, "Thermodynamic properties of lattice hard-sphere models", J. Chem. Phys. 123, 104504 (2005)
  2. Heitor C. Marques Fernandes, Jeferson J. Arenzon, and Yan Levin "Monte Carlo simulations of two-dimensional hard core lattice gases" J. Chem. Phys. 126, 114508 (2007).