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024 7 _ |a 10.1103/PhysRevB.81.235133
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|a Physics, Condensed Matter
100 1 _ |a Liebsch, A.
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245 _ _ |a Spectral weight of doping-induced states in the two-dimensional Hubbard model
260 _ _ |a College Park, Md.
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|c 2010
300 _ _ |a 235133
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440 _ 0 |a Physical Review B
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500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a The spectral weight of states induced in the Mott gap via hole doping in the two-dimensional Hubbard model is studied within cluster dynamical mean-field theory combined with finite-temperature exact diagonalization. If the cutoff energy is chosen to lie just below the upper Hubbard band, the integrated weight per spin is shown to satisfy W+(delta) >= delta (delta denotes the total number of holes), in agreement with model predictions by Eskes et al. [Phys. Rev. Lett. 67, 1035 (1991)]. However, if the cutoff energy is chosen to lie in the range of the pseudogap, W+(delta) remains much smaller than delta and approximately saturates near delta approximate to 0.2, ..., 0.3. The analysis of recent x-ray absorption spectroscopy data therefore depends crucially on the appropriate definition of the integration window.
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773 _ _ |a 10.1103/PhysRevB.81.235133
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