Metal-insulator transition in correlated systems: A new numerical approach
We study the Mott transition in the Hubbard model within the dynamical mean field theory approach where the density matrix renormalization group method is used to solve its self-consistent equations. The DMRG technique solves the associated impurity problem. We obtain accurate estimates of the criti...
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| Formato: | Capítulo de libro |
| Lenguaje: | Inglés |
| Publicado: |
2007
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| Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
| Aporte de: | Registro referencial: Solicitar el recurso aquí |
| LEADER | 05362caa a22008057a 4500 | ||
|---|---|---|---|
| 001 | PAPER-6426 | ||
| 003 | AR-BaUEN | ||
| 005 | 20250505094045.0 | ||
| 008 | 190411s2007 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-34447498537 | |
| 030 | |a PHYBE | ||
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a García, D.J. | |
| 245 | 1 | 0 | |a Metal-insulator transition in correlated systems: A new numerical approach |
| 260 | |c 2007 | ||
| 270 | 1 | 0 | |m Hallberg, K.; Instituto Balseiro, Centro Atómico Bariloche, CNEA, 8400 San Carlos de Bariloche, Argentina; email: karen@cab.cnea.gov.ar |
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| 504 | |a García, D., Miranda, E., Hallberg, K., Rozenberg, M., (2007) Phys. Rev. B, 75, pp. 121102R | ||
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| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a We study the Mott transition in the Hubbard model within the dynamical mean field theory approach where the density matrix renormalization group method is used to solve its self-consistent equations. The DMRG technique solves the associated impurity problem. We obtain accurate estimates of the critical values of the metal-insulator transitions. For the Hubbard model away from the particle-hole symmetric case we focus our study on the region of strong interactions and finite doping where two solutions coexist. In this region we demonstrate the capabilities of this method by obtaining the frequency-dependent optical conductivity spectra. With this algorithm, more complex models having a larger number of degrees of freedom can be considered and finite-size effects can be minimized. © 2007 Elsevier B.V. All rights reserved. |l eng | |
| 593 | |a Instituto de Física Gleb Wataghin, Unicamp, CEP 13083-970 Campinas, SP, Brazil | ||
| 593 | |a Instituto Balseiro, Centro Atómico Bariloche, CNEA, 8400 San Carlos de Bariloche, Argentina | ||
| 593 | |a Laboratoire de Physique des Solides, CNRS-UMR8502, Université de Paris-Sud, Orsay, 91405, France | ||
| 593 | |a Departamento de Física, FCEN, Universidad de Buenos Aires, Pabellón 1, Buenos Aires (1428), Argentina | ||
| 690 | 1 | 0 | |a DENSITY MATRIX RENORMALIZATION GROUP |
| 690 | 1 | 0 | |a DYNAMICAL MEAN FIELD THEORY |
| 690 | 1 | 0 | |a MOTT TRANSITION |
| 690 | 1 | 0 | |a DENSITY MATRIX RENORMALIZATION GROUPS |
| 690 | 1 | 0 | |a DYNAMICAL MEAN FIELD THEORY |
| 690 | 1 | 0 | |a MOTT TRANSITIONS |
| 690 | 1 | 0 | |a SELF-CONSISTENT EQUATIONS |
| 690 | 1 | 0 | |a DEGREES OF FREEDOM (MECHANICS) |
| 690 | 1 | 0 | |a MATRIX ALGEBRA |
| 690 | 1 | 0 | |a MEAN FIELD THEORY |
| 690 | 1 | 0 | |a OPTICAL CONDUCTIVITY |
| 690 | 1 | 0 | |a SEMICONDUCTOR DOPING |
| 690 | 1 | 0 | |a SPECTRUM ANALYSIS |
| 690 | 1 | 0 | |a METAL INSULATOR BOUNDARIES |
| 700 | 1 | |a Miranda, E. | |
| 700 | 1 | |a Hallberg, Karen Astrid | |
| 700 | 1 | |a Rozenberg, M.J. | |
| 773 | 0 | |d 2007 |g v. 398 |h pp. 407-411 |k n. 2 |p Phys B Condens Matter |x 09214526 |w (AR-BaUEN)CENRE-279 |t Physica B: Condensed Matter | |
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| 856 | 4 | 0 | |u https://doi.org/10.1016/j.physb.2007.04.049 |y DOI |
| 856 | 4 | 0 | |u https://hdl.handle.net/20.500.12110/paper_09214526_v398_n2_p407_Garcia |y Handle |
| 856 | 4 | 0 | |u https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_09214526_v398_n2_p407_Garcia |y Registro en la Biblioteca Digital |
| 961 | |a paper_09214526_v398_n2_p407_Garcia |b paper |c PE | ||
| 962 | |a info:eu-repo/semantics/article |a info:ar-repo/semantics/artículo |b info:eu-repo/semantics/publishedVersion | ||
| 963 | |a VARI | ||
| 999 | |c 67379 | ||