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Volumn 58, Issue 22, 1998, Pages R14685-R14688

Phase separation in the two-dimensional Hubbard model: A fixed-node quantum Monte Carlo study

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Indexed keywords


EID: 0000278478     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.58.R14685     Document Type: Article
Times cited : (40)

References (31)
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    • 0001283374 scopus 로고    scopus 로고
    • Gang Su, Phys. Rev. B 54, R8281 (1996).
    • (1996) Phys. Rev. B , vol.54 , pp. R8281
  • 28
    • 0004071284 scopus 로고
    • This term was proposed long ago by Takahashi, J. Phys. C 10, 1289 (1977).
    • (1977) J. Phys. C , vol.10 , pp. 1289
  • 29
    • 0542429623 scopus 로고    scopus 로고
    • the resulting large-(Formula presented) expansion agrees remarkably well, for U⩾10, with the more recent results of G. Polatsek and K. W. Becker, Phys. Rev. B 54, 1637 (1996).
    • (1996) Phys. Rev. B , vol.54 , pp. 1637
    • Polatsek, G.1    Becker, K.2
  • 30
    • 0000885142 scopus 로고
    • The Gutzwiller-Slater wave function, a very popular choice for the Hubbard model, suffers from at least two drawbacks (which probably reflect into the “quality” of its nodes): it does not describe a spin singlet and it only has on-site correlations; we are presently trying out more general forms, such as those proposed by T. Giamarchi and C. Lhuillier, Phys. Rev. B 42, 10 641 (1990).
    • (1990) Phys. Rev. B , vol.42 , pp. 10641
    • Giamarchi, T.1    Lhuillier, C.2
  • 31
    • 0039312913 scopus 로고
    • In a finite L×L lattice even for (Formula presented) the energy of a tight-binding system would show an artificial phase separation at (Formula presented), due to the high degeneracy at the Fermi level: see H. Q. Lin, Phys. Rev. B 44, 7151 (1991).
    • (1991) Phys. Rev. B , vol.44 , pp. 7151
    • Lin, H.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.