Idealised models: Difference between revisions
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__NOTOC__ | __NOTOC__ | ||
==Lattice models== | ==Lattice models== | ||
*[[Bond fluctuation model]] | |||
*[[Hard hexagons]] | *[[Hard hexagons]] | ||
*[[Heisenberg model]] | *[[Heisenberg model]] | ||
*[[Ising Models]] | *[[Ising Models]] | ||
*[[ | *[[Kac model]] | ||
*[[Lattice gas]] | *[[Lattice gas]] | ||
*[[Lebwohl-Lasher model]] | *[[Lebwohl-Lasher model]] | ||
*[[Potts model]] | *[[Potts model]] | ||
*[[ | *[[RP(n-1) model]] | ||
*[[XY model]] | |||
=='Hard' models== | =='Hard' models== |
Revision as of 14:46, 25 September 2007
Lattice models
- Bond fluctuation model
- Hard hexagons
- Heisenberg model
- Ising Models
- Kac model
- Lattice gas
- Lebwohl-Lasher model
- Potts model
- RP(n-1) model
- XY model
'Hard' models
- Hard rods
- Hard disks
- Hard sphere
- Widom-Rowlinson model
- Two-dimensional hard dumbbells
- Three-dimensional hard dumbbells
- Tangent linear hard sphere chains
- Flexible hard sphere chains (also known as the pearl-necklace model)
- Branched hard sphere chains
- Fused hard sphere chains
- Hard ellipsoids
- Hard spherocylinders
- Hard core Yukawa
Piecewise continuous models
'Soft' models
- Gaussian overlap model
- Gay-Berne model
- Kihara potential
- Lennard-Jones rods
- Lennard-Jones disks
- Lennard-Jones model
- Lennard-Jones sticks
- 9-3 Lennard-Jones potential
- United-atom model
- Intermolecular Interactions
- Flexible molecules (intramolecular interactions)
- Confined systems
'Charged' models
- Restricted primitive model
- Charged hard dumbbells
- Shell model
- Relaxed shell model
- Dynamical shell model (also known as the adiabatic shell model)
Three-body potentials
- Axilrod-Teller interaction
- Silicon
- Many-body interactions - a general discussion page.