Competition between d-wave superconductivity and antiferromagnetism in the two-dimensional Hubbard model (Articolo in rivista)

Type
Label
  • Competition between d-wave superconductivity and antiferromagnetism in the two-dimensional Hubbard model (Articolo in rivista) (literal)
Anno
  • 2006-01-01T00:00:00+01:00 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
  • 10.1103/PhysRevB.74.054513 (literal)
Alternative label
  • Massimo Capone; Gabriel Kotliar (2006)
    Competition between d-wave superconductivity and antiferromagnetism in the two-dimensional Hubbard model
    in Physical review. B, Condensed matter and materials physics; The American Physical Society, Ridge, NY (Stati Uniti d'America)
    (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#autori
  • Massimo Capone; Gabriel Kotliar (literal)
Pagina inizio
  • 054513 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#url
  • http://prb.aps.org/abstract/PRB/v74/i5/e054513 (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroVolume
  • 74 (literal)
Rivista
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#numeroFascicolo
  • 5 (literal)
Note
  • ISI Web of Science (WOS) (literal)
Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#affiliazioni
  • INFM SMC, I-00185 Rome, Italy; CNR, Ist Sistemi Complessi, I-00185 Rome, Italy; Univ Roma La Sapienza, Phys Dept, I-00185 Rome, Italy; Rutgers State Univ, Phys Dept, Piscataway, NJ 08854 USA; Rutgers State Univ, Ctr Mat Theory, Piscataway, NJ 08854 USA (literal)
Titolo
  • Competition between d-wave superconductivity and antiferromagnetism in the two-dimensional Hubbard model (literal)
Abstract
  • We study the competition of antiferromagnetism and d-wave superconductivity at zero temperature in the two-dimensional Hubbard model using cellular dynamical mean-field theory for a 2x2 plaquette, and solve the associated cluster impurity model at zero temperature by means of exact diagonalization. The interplay between the two phases depends strongly on the strength of the correlation. At strong coupling (U greater than or similar to 8t) the two phases do not mix, and a first-order transition takes place as a function of doping between two pure phases. At weak coupling (U less than or similar to 8t) the two order parameters coexist within the same solution in a range of doping and the system smoothly evolves from the antiferromagnet to the superconductor. When the transition between the superconducting and the antiferromagetic phases is of the first-order, it is accompanied by a phase separation. (literal)
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