Home > Publications database > Non-Fermi-liquid phases in the two-band Hubbard model: Finite-temperature exact diagonalization study of Hund's rule coupling > print |
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024 | 7 | _ | |2 DOI |a 10.1140/epjb/e2006-00248-0 |
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041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
100 | 1 | _ | |0 P:(DE-Juel1)VDB941 |a Liebsch, A. |b 0 |u FZJ |
245 | _ | _ | |a Non-Fermi-liquid phases in the two-band Hubbard model: Finite-temperature exact diagonalization study of Hund's rule coupling |
260 | _ | _ | |a Berlin |b Springer |c 2006 |
300 | _ | _ | |a 523 |
336 | 7 | _ | |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |a Journal Article |
336 | 7 | _ | |2 DataCite |a Output Types/Journal article |
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336 | 7 | _ | |2 BibTeX |a ARTICLE |
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336 | 7 | _ | |2 DRIVER |a article |
440 | _ | 0 | |0 1982 |a European Physical Journal B |v 51 |x 1434-6028 |
500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
520 | _ | _ | |a The two-band Hubbard model involving subbands of different widths is investigated via finite-temperature exact diagonalization (ED) and dynamical mean field theory (DMFT). In contrast to the quantum Monte Carlo (QMC) method which at low temperatures includes only Ising-like exchange interactions to avoid sign problems, ED permits a treatment of Hund's exchange and other onsite Coulomb interactions on the same footing. The role of finite-size effects caused by the limited number of bath levels in this scheme is studied by analyzing the low-frequency behavior of the subband self-energies as a function of temperature, and by comparing with numerical renormalization group (NRG) results for a simplified effective model. For half-filled, non-hybridizing bands, the metallic and insulating phases are separated by an intermediate mixed phase with an insulating narrow and a bad-metallic wide subband. The wide band in this phase exhibits different degrees of non-Fermi-liquid behavior, depending on the treatment of exchange interactions. Whereas for complete Hund's coupling, infinite lifetime is found at the Fermi level, in the absence of spin-flip and pair-exchange, this lifetime becomes finite. Excellent agreement is obtained both with new NRG and previous QMC/DMFT calculations. These results suggest that-finite temperature ED/DMFT might be a useful scheme for realistic multi-band materials. |
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700 | 1 | _ | |0 P:(DE-Juel1)130600 |a Costi, T. A. |b 1 |u FZJ |
773 | _ | _ | |0 PERI:(DE-600)1459068-2 |a 10.1140/epjb/e2006-00248-0 |g Vol. 51, p. 523 |p 523 |q 51<523 |t The @European physical journal / B |v 51 |x 1434-6028 |y 2006 |
856 | 7 | _ | |u http://dx.doi.org/10.1140/epjb/e2006-00248-0 |
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