Incommensurability and edge states in the one-dimensional S=1 bilinear-biquadratic model

dc.creatorMurashima, Takahiro
dc.creatorNomura, Kiyohide
dc.date2006-02-14
dc.date2006-05-02
dc.date.accessioned2026-07-07T07:01:43Z
dc.date.available2026-07-07T07:01:43Z
dc.descriptionCommensurate-incommensurate change on the one-dimensional S=1 bilinear-biquadratic model (${\cal H}(α)=\sum_i \{{\bf S}_i\cdot {\bf S}_{i+1} +α({\bf S}_i\cdot{\bf S}_{i+1})^2\}$) is examined. The gapped Haldane phase has two subphases (the commensurate Haldane subphase and the incommensurate Haldane subphase) and the commensurate-incommensurate change point (the Affleck-Kennedy-Lieb-Tasaki point, $α=1/3$). There have been two different analytical predictions about the static structure factor in the neighborhood of this point. By using the Sørensen-Affleck prescription, these static structure factors are related to the Green functions, and also to the energy gap behaviors. Numerical calculations support one of the predictions. Accordingly, the commensurate-incommensurate change is recognized as a motion of a pair of poles in the complex plane.
dc.description29 pages, 15 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0602336
dc.identifierhttp://arxiv.org/abs/cond-mat/0602336
dc.identifierPhys. Rev. B, Vol. 73, p.214431 (2006)
dc.identifierdoi:10.1103/PhysRevB.73.214431
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/108359
dc.subjectStrongly Correlated Electrons
dc.titleIncommensurability and edge states in the one-dimensional S=1 bilinear-biquadratic model
dc.typetext

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