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Magnetic and charge structures in itinerant-electron magnets: Coexistence of multiple spin-density and charge-density waves

2001/08/17 by Fusayoshi J. Ohkawa · 2 citations
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Magnetic and transport properties of perovskites and related materials #Physics of Superconductivity and Magnetism #cond-mat.str-el

paper · pdf · doi:10.1103/physrevb.66.014408

10 pages, no figures

arxiv created 2001/08/17 · openalex publication_date 2002/06/26 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28

Abstract

A theory of Kondo lattices is applied to studying possible magnetic and charge structures of itinerant-electron antiferromagnets. Even helical spin structures can be stabilized when the nesting of the Fermi surface is not sharp and the superexchange interaction, which arises from the virtual exchange of pair excitations across the Mott-Hubbard gap, is mainly responsible for magnetic instability. Sinusoidal spin structures or spin-density waves (SDW's) are only stabilized when the nesting of the Fermi surface is sharp enough or when an exchange interaction arising from that of pair excitations of quasiparticles is mainly responsible for magnetic instability. In particular, multiple SDW's are stabilized when their incommensurate ordering wave numbers \ifmmode±\else\textpm\fiQ are multiple; magnetizations of different \ifmmode±\else\textpm\fiQ components are orthogonal to each other in double and triple SDW's when magnetic anisotropy is weak enough. Unless \ifmmode±\else\textpm\fi2Q are commensurate, charge-density waves (CDW's) with \ifmmode±\else\textpm\fi2Q coexist with SDW's with \ifmmode±\else\textpm\fiQ. Because the quenching of magnetic moments by the Kondo effect or local quantum spin fluctuations depends on local numbers of electrons, the phase of CDW's or electron densities is such that magnetic moments are large where the quenching is weak. It is proposed that the so-called stripe order must be the coexisting state of double incommensurate SDW's and CDW's in tetragonal cuprate-oxide high temperature superconductors, in particular, those with the square CuO2 lattices.

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