Math 2.0

Statistical mechanics, structure of matter Lattice spin systems Example

ANNNI model

Builds on Ising model

Example

Let Λ\Lambda be a finite box of ℤd\Z^d and pick one coordinate axis, the axial direction. Let J0,J1>0J_0, J_1 > 0 and J2>0J_2 > 0 be constants and let β≥0\beta \ge 0 be the inverse temperature. A configuration is σ ⁣:Λ→{−1,+1}\sigma \colon \Lambda \to \set{-1, +1}, and ee denotes the unit vector of the axial direction. Its energy is H(σ)=−J0∑in-layerσxσy−J1∑xσxσx+e+J2∑xσxσx+2e,H(\sigma) = -J_0 \sum_{\text{in-layer}} \sigma_x \sigma_y - J_1 \sum_{x} \sigma_x \sigma_{x + e} + J_2 \sum_{x} \sigma_x \sigma_{x + 2e}, where the first sum runs over nearest-neighbour pairs {x,y}\set{x, y} with y−xy - x orthogonal to ee. The ANNNI model (axial next-nearest-neighbour Ising model) is the probability measure on {−1,+1}Λ\set{-1, +1}^\Lambda proportional to e−βH(σ)e^{-\beta H(\sigma)}.

Remarks

The nearest-neighbour terms favour alignment, while the next-nearest-neighbour axial term with J2>0J_2 > 0 favours opposite spins at distance two, so the interactions compete. At zero temperature, along one axial chain the ferromagnetic pattern has energy −J1+J2-J_1 + J_2 per site and the pattern ++−−++-- has energy −J2-J_2 per site. So the ground state is ferromagnetic when J2/J1<1/2J_2 / J_1 < 1/2 and of type ++−−++-- when J2/J1>1/2J_2 / J_1 > 1/2. At positive temperature the model shows many modulated phases with different periods along the axis. For J2=0J_2 = 0 it is an anisotropic Ising model with couplings J0J_0 and J1J_1.

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Further reading

  1. Web https://en.wikipedia.org/wiki/ANNNI_model
About this page
Tag36Y0AM16EB
URIm2://36Y0AM16EB
Kindexample
WritingW0 stub
MSC82B20, 82D40
Instance ofLattice model
UsesIsing model
Same as
Changed3 November 2026

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