Heisenberg model: Difference between revisions

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The '''Heisenberg model''' is the n=3 case of the ''n''-vector model. The [[Hamiltonian]] is given by
:<math>H = -J{\sum}_{\langle i,j\rangle}\mathbf{S}_i \cdot \mathbf{S}_{j}</math>
where the sum runs over all pairs of nearest neighbour spins, <math>\mathbf{S}</math>, and where <math>J</math> is the coupling constant.
==See also==
==See also==
*[[Ising Models]] (n=1)
*[[XY model]] (n=2)
*[[Mermin-Wagner theorem]]
*[[Mermin-Wagner theorem]]
==References==
==References==

Revision as of 16:23, 22 January 2008

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The Heisenberg model is the n=3 case of the n-vector model. The Hamiltonian is given by

where the sum runs over all pairs of nearest neighbour spins, , and where is the coupling constant.

See also

References

  1. A. C. Hewson and D. Ter Haar "On the theory of the Heisenberg ferromagnet", Physica 30 pp. 271-276 (1964)
  2. T. M. Giebultowicz and J. K. Furdyna "Monte Carlo simulation of fcc Heisenberg antiferromagnet with nearest- and next-nearest-neighbor interactions", Journal of Applied Physics 57 pp. 3312-3314 (1985)
  3. F. Lado and E. Lomba "Heisenberg Spin Fluid in an External Magnetic Field ", Physical Review Letters 80 pp. 3535-3538 (1998)
  4. E. Lomba, C. Martín and N.G. Almarza "Theory and simulation of positionally frozen Heisenberg spin systems", The European Physical Journal B 34 pp. 473-478 (2003)