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Role of next-nearest-neighbor hopping in the [ital t]-[ital t][prime]-[ital J] model

Journal Article · · Physical Review, B: Condensed Matter; (United States)
 [1];  [2]
  1. Max-Planck-Institut fuer Physik komplexer System, Aussenstelle Stuttgart, Heisenbergstrasse 1, D-70569 Stuttgart (Germany)
  2. Department of Applied Physics, Nagoya University, Nagoya 464-01 (Japan)
A next-nearest-neighbor hopping [ital t][prime] in the [ital t]-[ital t][prime]-[ital J] model has a different sign between the hole- and electron-doped systems of high-[ital T][sub [ital c]] cuprates: [ital t][prime][lt]0 for the hole-doped system and [ital t][prime][gt]0 for the electron-doped system. We show that the sign is responsible for the remarkable difference of antiferromagnetic (AF) phases between the two systems. To reveal this and clarify the role of [ital t][prime], we examine magnetic excitations of the [ital t]-[ital t][prime]-[ital J] model by employing exact diagonalization techniques for 4[times]4 and [radical]18 [times] [radical]18 lattices. In the low-doping region (two-hole case of the [radical]18 [times] [radical]18 lattice), AF spin correlations are stabilized for the case of [ital t][prime][gt]0, i.e., electron-doping case, but not for the case of [ital t][prime][lt]0. In the high-doping region (four-hole case of the 4[times]4 lattice and more) magnetic excitations are mainly controlled by the geometry of the Fermi surface of the noninteracting system.
OSTI ID:
5222490
Journal Information:
Physical Review, B: Condensed Matter; (United States), Journal Name: Physical Review, B: Condensed Matter; (United States) Vol. 49:5; ISSN PRBMDO; ISSN 0163-1829
Country of Publication:
United States
Language:
English

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