We study the doping-driven Mott metal-insulator transition (MIT) in the periodic Anderson model set in the Mott-Hubbard regime. A striking asymmetry for electron- or hole-driven transitions is found. The electron-doped MIT at larger U is similar to the one found in the single band Hubbard model, with a first-order character due to coexistence of solutions. The hole-doped MIT, in contrast, is second order and can be described as the delocalization of Zhang-Rice singlets.

Asymmetry between the electron- and hole-doped Mott transition in the periodic Anderson model / Sordi, G.; Amaricci, A.; Rozenberg, M. J.. - In: PHYSICAL REVIEW. B, CONDENSED MATTER AND MATERIALS PHYSICS. - ISSN 1098-0121. - 80:3(2009), pp. 1-15. [10.1103/PhysRevB.80.035129]

Asymmetry between the electron- and hole-doped Mott transition in the periodic Anderson model

Amaricci, A.;
2009-01-01

Abstract

We study the doping-driven Mott metal-insulator transition (MIT) in the periodic Anderson model set in the Mott-Hubbard regime. A striking asymmetry for electron- or hole-driven transitions is found. The electron-doped MIT at larger U is similar to the one found in the single band Hubbard model, with a first-order character due to coexistence of solutions. The hole-doped MIT, in contrast, is second order and can be described as the delocalization of Zhang-Rice singlets.
2009
80
3
1
15
035129
https://journals.aps.org/prb/abstract/10.1103/PhysRevB.80.035129
https://arxiv.org/abs/0906.4777
Sordi, G.; Amaricci, A.; Rozenberg, M. J.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11767/32398
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