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Volumn 44, Issue 17, 1991, Pages 9410-9417

Fixed-node Monte Carlo study of the two-dimensional Hubbard model

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Indexed keywords


EID: 0038858927     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.44.9410     Document Type: Article
Times cited : (32)

References (22)
  • 15
    • 84927823323 scopus 로고    scopus 로고
    • In continuous space, F would have to be chosen as exp (- τ H) or (H -w)-1 due to the need for F to be a bounded operator.
  • 17
    • 84927823322 scopus 로고    scopus 로고
    • Other continuation of the wave function ψ (R) outside the region V is conceivable. For example, one could take ψ (R)= ψT(R) for R member V. The problem is that we no longer have an eigenvalue equation.
  • 19
    • 84927823321 scopus 로고    scopus 로고
    • In the continuum case, we have H ψ hat (R) = curlep ψ hat (R), except on the nodal surface where ψT(R) =0. The second term in the right-hand side of (36) does not appear. Hence EF= curlep = E. The equality EF=E guarantees that EF is an upper bound to the true ground-state energy, while in the discrete case (35) remains a so-called mixed estimator of the ground-state energy since H is sandwiched between two different states. A general inequality between EF and the true ground-state energy could not be established in the discrete case.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.