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000052189 084__ $$2WoS$$aPhysics, Condensed Matter
000052189 1001_ $$0P:(DE-HGF)0$$aSangiovanni, G.$$b0
000052189 245__ $$aStatic versus dynamical mean-field theory of Mott antiferromagnets
000052189 260__ $$aCollege Park, Md.$$bAPS$$c2006
000052189 300__ $$a205121
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000052189 440_0 $$04919$$aPhysical Review B$$v73$$x1098-0121
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000052189 520__ $$aStudying the antiferromagnetic phase of the Hubbard model by dynamical mean-field theory, we observe striking differences with static (Hartree-Fock) mean field: The Slater band is strongly renormalized and spectral weight is transferred to spin-polaron sidebands. Already for intermediate values of the interaction U the overall bandwidth is larger than in the Hartree-Fock mean field and the gap is considerably smaller. Such differences survive any renormalization of U. Our photoemission experiments for Cr-doped V2O3 show spectra qualitatively well described by dynamical mean-field theory.
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000052189 7001_ $$0P:(DE-HGF)0$$aToschi, A.$$b1
000052189 7001_ $$0P:(DE-Juel1)VDB43156$$aKoch, E.$$b2$$uFZJ
000052189 7001_ $$0P:(DE-HGF)0$$aHeld, K.$$b3
000052189 7001_ $$0P:(DE-HGF)0$$aCapone, M.$$b4
000052189 7001_ $$0P:(DE-HGF)0$$aCastellani, C.$$b5
000052189 7001_ $$0P:(DE-HGF)0$$aGunnarsson, O.$$b6
000052189 7001_ $$0P:(DE-HGF)0$$aMo, S.-K.$$b7
000052189 7001_ $$0P:(DE-HGF)0$$aAllen, J. W.$$b8
000052189 7001_ $$0P:(DE-HGF)0$$aKim, H.-D.$$b9
000052189 7001_ $$0P:(DE-HGF)0$$aSekiyama, A.$$b10
000052189 7001_ $$0P:(DE-HGF)0$$aYamasaki, A.$$b11
000052189 7001_ $$0P:(DE-HGF)0$$aSuga, S.$$b12
000052189 7001_ $$0P:(DE-HGF)0$$aMetcalf, P.$$b13
000052189 77318 $$2Crossref$$3journal-article$$a10.1103/physrevb.73.205121$$bAmerican Physical Society (APS)$$d2006-05-31$$n20$$p205121$$tPhysical Review B$$v73$$x1098-0121$$y2006
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000052189 8567_ $$uhttp://hdl.handle.net/2128/1445$$uhttp://dx.doi.org/10.1103/PhysRevB.73.205121
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