Idealised models: Difference between revisions
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Carl McBride (talk | contribs) |
Carl McBride (talk | contribs) m (→Lattice models) |
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*[[Bond fluctuation model]] | *[[Bond fluctuation model]] | ||
*[[Hard hexagons]] | *[[Hard hexagons]] | ||
*[[Kac model]] | *[[Kac model]] | ||
*[[Lattice gas]] | *[[Lattice gas]] | ||
| Line 12: | Line 10: | ||
*[[Potts model]] | *[[Potts model]] | ||
*[[RP(n-1) model]] | *[[RP(n-1) model]] | ||
*[[XY model]] | *N-vector model: | ||
**[[Ising Models]] (n=1) | |||
**[[XY model]] (n=2) | |||
**[[Heisenberg model]] (n=3) | |||
=='Hard' models== | =='Hard' models== | ||
Revision as of 17:04, 22 January 2008
Lattice models
- Barker-Fock model
- Blume-Emery-Griffiths model (including the Blume-Capel model)
- Bond fluctuation model
- Hard hexagons
- Kac model
- Lattice gas
- Lebwohl-Lasher model
- Potts model
- RP(n-1) model
- N-vector model:
- Ising Models (n=1)
- XY model (n=2)
- Heisenberg model (n=3)
'Hard' models
- Branched hard sphere chains
- Flexible hard sphere chains (also known as the pearl-necklace model)
- Fused hard sphere chains
- Hard core Yukawa
- Hard disks
- Hard dumbbell model
- Hard ellipsoids
- Hard rods
- Hard sphere
- Hard spherocylinders
- Tangent linear hard sphere chains
- Widom-Rowlinson model
Piecewise continuous models
'Soft' models
- 9-3 Lennard-Jones potential
- 10-4-3 Lennard-Jones potential
- Confined systems
- Flexible molecules (intramolecular interactions)
- Gaussian overlap model
- Gay-Berne model
- Intermolecular Interactions
- Kihara potential
- Lennard-Jones disks
- Lennard-Jones model
- Lennard-Jones rods
- Lennard-Jones sticks
- Morse potential
- United-atom model
'Charged' models
Three-body potentials
- Axilrod-Teller interaction
- Silicon
- Many-body interactions - a general discussion page.