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ising [2021/04/15 05:02] Scott Lawrence [Operator content] |
ising [2021/09/23 17:34] (current) Scott Lawrence [Fractional dimensions] |
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S = \sum_r \left[ J_x s_r s_{r+\hat x} + J_y s_r s_{r+\hat y} + J_z s_r s_{r+\hat z} \right] | S = \sum_r \left[ J_x s_r s_{r+\hat x} + J_y s_r s_{r+\hat y} + J_z s_r s_{r+\hat z} \right] | ||
\] | \] | ||
- | The case where $J_y = J_z \gg J_x$ is termed the Hamiltonian limit, as it is connected by the Suzuki-Trotter expansion (and the [[transfer matrix|transfer matrix]]) to a quantum mechanical system. | + | The case where $J_y = J_z \gg J_x$ is termed the Hamiltonian limit, as it is connected by the Suzuki-Trotter expansion (and the [[transfer matrix|transfer matrix]]) to a quantum mechanical system, usually termed the " |
\[ | \[ | ||
H = -\mu \sum_i \sigma_x(i) -J \sum_{\langle i j \rangle} \sigma_z(i) \sigma_z(j) | H = -\mu \sum_i \sigma_x(i) -J \sum_{\langle i j \rangle} \sigma_z(i) \sigma_z(j) | ||
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The two-dimensional lattice Ising model was solved exactly by Onsager. | The two-dimensional lattice Ising model was solved exactly by Onsager. | ||
+ | The Hamiltonian limit of this model is a spin chain (referred to as the " | ||
+ | \[ | ||
+ | H = -\mu \sum_r \sigma_x(r) - J \sum_r \sigma_z(r) \sigma_z(r+1)\text. | ||
+ | \] | ||
+ | This model can be transformed to a quadratic theory of fermion fields, and thence solved, via a Jordan-Wigner transformation. | ||
==== Higher dimensions ==== | ==== Higher dimensions ==== | ||
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[[https:// | [[https:// | ||
+ | |||
+ | [[https:// | ||
===== External links ===== | ===== External links ===== | ||
* [[https:// | * [[https:// | ||
* [[https:// | * [[https:// |