In condensed matter physics, an AKLT model, also known as an Affleck-Kennedy-Lieb-Tasaki model is an extension of the one-dimensional quantum Heisenberg spin model. The proposal and exact solution of this model by Ian Affleck, Elliott H. Lieb, Tom Kennedy and Hal Tasaki [ja][1] provided crucial insight into the physics of the spin-1 Heisenberg chain.[2][3][4][5] It has also served as a useful example for such concepts as valence bond solid order, symmetry-protected topological order[6][7][8][9] and matrix product state wavefunctions.
^Cite error: The named reference Affleck:1987 was invoked but never defined (see the help page).
^Haldane, F. D. M. (1983). "Nonlinear Field Theory of Large-Spin Heisenberg Antiferromagnets: Semiclassically Quantized Solitons of the One-Dimensional Easy-Axis Néel State". Phys. Rev. Lett. 50 (15): 1153. Bibcode:1983PhRvL..50.1153H. doi:10.1103/physrevlett.50.1153.
^Haldane, F. D. M. (1983). "Continuum dynamics of the 1-D Heisenberg antiferromagnet: Identification with the O(3) nonlinear sigma model". Phys. Lett. A. 93 (9): 464. Bibcode:1983PhLA...93..464H. doi:10.1016/0375-9601(83)90631-x.
^Affleck, I.; Haldane, F. D. M. (1987). "Critical theory of quantum spin chains". Phys. Rev. B. 36 (10): 5291–5300. Bibcode:1987PhRvB..36.5291A. doi:10.1103/physrevb.36.5291. PMID 9942166.
^Affleck, I. (1989). "Quantum spin chains and the Haldane gap". J. Phys.: Condens. Matter. 1 (19): 3047. Bibcode:1989JPCM....1.3047A. doi:10.1088/0953-8984/1/19/001. S2CID 250850599.
physics, an AKLTmodel, also known as an Affleck-Kennedy-Lieb-Tasaki model is an extension of the one-dimensional quantum Heisenberg spin model. The proposal...
\end{bmatrix}}\quad A_{3}={\begin{bmatrix}|1\rangle &0\\0&|0\rangle \end{bmatrix}}.} The AKLT ground state wavefunction, which is the historical example of MPS approach:...
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