Bosonic representation of spin operators in the field-induced critical phase of spin-1 Haldane chains

Details Bosonic representation of spin operators in the field-induced critical phase of spin-1 Haldane chains Bosonic representation of spin operators in the field-induced critical phase of spin-1 Haldane chains

2006-05-25

arxiv.org/abs/cond-mat/0605636v3

Journal of Statistical Mechanics: Theory and Experiment (2006) P09001

Physics

Condensed Matter

Strongly Correlated Electrons

31 pages (1 column), 1 figure, published version

Scientific paper

10.1088/1742-5468/2006/09/P09001

A bosonized-field-theory representation of spin operators in the uniform-field-induced Tomonaga-Luttinger-liquid (TLL) phase in spin-1 Haldane chains is formulated by means of the non-Abelian (Tsvelik's Majorana fermion theory) and the Abelian bosonizations and Furusaki-Zhang technique [Phys. Rev. B {\bf 60}, 1175 (1999)]. It contains massive magnon fields as well as massless boson fields. From it, asymptotic forms of spin correlation functions in the TLL phase are completely determined. Applying the formula, we further discuss effects of perturbations (bond alternation, single-ion anisotropy terms, staggered fields, etc) for the TLL state, and the string order parameter. Throughout the paper, we often consider in some detail how the symmetry operations of the Haldane chains are translated in the low-energy effective theory.

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