Metal-insulator transitions in the periodic Anderson model

We solve the periodic Anderson model in the Mott-Hubbard regime, using dynamical mean field theory. Upon electron doping of the Mott insulator, a metal-insulator transition occurs which is qualitatively similar to that of the single band Hubbard model, namely, with a divergent effective mass and a f...

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Autor principal: Sordi, G.
Otros Autores: Amaricci, A., Rozenberg, M.J
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2007
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
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100 1 |a Sordi, G. 
245 1 0 |a Metal-insulator transitions in the periodic Anderson model 
260 |c 2007 
270 1 0 |m Sordi, G.; Laboratoire de Physique des Solides, CNRS-UMR8502, Université de Paris-Sud, Orsay 91405, France 
506 |2 openaire  |e Política editorial 
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504 |a Georges, A., Krauth, W., (1993) Phys. Rev. B, 48, p. 7167. , PRBMDO 0163-1829 10.1103/PhysRevB.48.7167 
504 |a Rozenberg, M.J., Kotliar, G., Zhang, X.Y., (1994) Phys. Rev. B, 49, p. 10181. , PRBMDO 0163-1829 10.1103/PhysRevB.49.10181 
504 |a Rozenberg, M.J., Chitra, R., Kotliar, G., (1999) Phys. Rev. Lett., 83, p. 3498. , PRLTAO 0031-9007 10.1103/PhysRevLett.83.3498 
504 |a Kotliar, G., Lange, E., Rozenberg, M.J., (2000) Phys. Rev. Lett., 84, p. 5180. , PRLTAO 0031-9007 10.1103/PhysRevLett.84.5180 
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504 |a Limelette, P., (2003) Phys. Rev. Lett., 91, p. 016401. , PRLTAO 0031-9007 10.1103/PhysRevLett.91.016401 
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504 |a Kotliar, G., Vollhardt, D., (2004) Phys. Today, 57 (3), p. 53. , PHTOAD 0031-9228 10.1063/1.1712502 
504 |a Kotliar, G., (2006) Rev. Mod. Phys., 78, p. 865. , RMPHAT 0034-6861 10.1103/RevModPhys.78.865 
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520 3 |a We solve the periodic Anderson model in the Mott-Hubbard regime, using dynamical mean field theory. Upon electron doping of the Mott insulator, a metal-insulator transition occurs which is qualitatively similar to that of the single band Hubbard model, namely, with a divergent effective mass and a first order character at finite temperatures. Surprisingly, upon hole doping, the metal-insulator transition is not first order and does not show a divergent mass. Thus, the transition scenario of the single band Hubbard model is not generic for the periodic Anderson model, even in the Mott-Hubbard regime. © 2007 The American Physical Society.  |l eng 
593 |a Laboratoire de Physique des Solides, CNRS-UMR8502, Université de Paris-Sud, Orsay 91405, France 
593 |a Departamento de Física, FCEN, Ciudad Universitaria Pab. I, Buenos Aires (1428), Argentina 
690 1 0 |a DOPING (ADDITIVES) 
690 1 0 |a ELECTRONS 
690 1 0 |a HUBBARD MODEL 
690 1 0 |a MEAN FIELD THEORY 
690 1 0 |a THERMAL EFFECTS 
690 1 0 |a ANDERSON MODEL 
690 1 0 |a MOTT INSULATOR 
690 1 0 |a MOTT-HUBBARD REGIME 
690 1 0 |a HIGH ENERGY PHYSICS 
700 1 |a Amaricci, A. 
700 1 |a Rozenberg, M.J. 
773 0 |d 2007  |g v. 99  |k n. 19  |p Phys Rev Lett  |x 00319007  |w (AR-BaUEN)CENRE-386  |t Physical Review Letters 
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