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Titlebook: Concepts in Electron Correlation; Alex C. Hewson,Veljko Zlatić Book 2003 Springer Science+Business Media Dordrecht 2003 band structure.con

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Josephson Effect In The Cuprates: Microscopic Implications,sparency. In the cuprates, the experimental value of .... (../..) is much smaller (larger) than the BCS prediction. We argue that both peculiarities of the cuprates can be explained by postulating quantum fluctuations of the pairing symmetry.
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Towards Models of Magnetic Interactions in the Cuprates,isingly large c-axis dispersion due to hybridization with unoccupied cation .-states in the adjacent layers. Hence, they must have relevance to .-axis magnetic coupling. In view of this situation, the Emery model is incomplete for the description of magnetism of undoped cuprates.
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Spectral Functions and Pseudogap in a Model of Strongly Correlated Electrons,. Longer-range spin fluctuations induce a pseudogap showing up at low doping in the effective truncation of the Fermi surface and in reduced electron and quasiparticle density of states at the Fermi level.
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Quasiparticles in Photoemission Spectra of Manganites,spersion on the orbiton energy scale is modified by orbital polarization and by electron-lattice coupling. A lower QP dispersion and quantum decoherence are obtained due to the inter-planar hole-magnon scattering in the .AF phase which disproves the classical concept of a ferromagnetic polaron.
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Metals Near a Zero-Temperature Magnetic Instability,er Au concentration, hydrostatic pressure, or magnetic field. In the system UC..-.Pd., strong disorder affects the NFL properties. The d-electron Laves phase ZrZn. was recently found to display superconductivity in coexistence with itinerant ferromagnetism.
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Viktor L. Ginzburg,Boris Khesinand the optical intraband spectral weight along the plane. We show that the BCS-prediction produces the wrong sign for the kink at .. of the intraband spectral weight, even though the model calculation agrees well with the specific heat.
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Nucleation and Pinning of Vortices in 4He,ting samples — by application of uniaxial stress . The continuous stress tuning allows the observation of dynamic scaling of σ(.) and hence a reliable determination of the critical exponent . of the extrapolated zerotemperature conductivity σ(0) ~∣ . — .. ∣., i.e. . = 1, and of the dynamical exponent .
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