Considerations on the quantum double-exchange Hamiltonian
arXiv:cond-mat/0101234 · doi:10.1103/PhysRevB.64.054406
Abstract
Schwinger bosons allow for an advantageous representation of quantum double-exchange. We review this subject, comment on previous results, and address the transition to the semiclassical limit. We derive an effective fermionic Hamiltonian for the spin-dependent hopping of holes interacting with a background of local spins, which is used in a related publication within a two-phase description of colossal magnetoresistant manganites.
7 pages, 3 figures
References in corpus (6)
- Calculation of Densities of States and Spectral Functions by Chebyshev Recursion and Maximum Entropy
- Electronic Hamiltonian for Transition Metal Oxide Compounds
- Optical absorption and single-particle excitations in the 2D Holstein t-J model
- Temperature dependence of the resistivity in the double-exchange model
- Phase diagram of an extended Kondo lattice model for manganites: the Schwinger-boson mean-field approach
- spl(2,1) dynamical supersymmetry and suppression of ferromagnetism in flat band double-exchange models
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