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Volumn 81, Issue 1, 2010, Pages

Gutzwiller magnetic phase diagram of the undoped t- t′ -U Hubbard model

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EID: 77954796048     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.014510     Document Type: Article
Times cited : (19)

References (24)
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    • Part of this difference is due to the fact that the RPA calculation samples all q values [Fig. ] while the Gutzwiller calculation was restricted to the high-symmetry axes, Γ→ (π,0 ) → (π,π ) →Γ
    • Part of this difference is due to the fact that the RPA calculation samples all q values [Fig.] while the Gutzwiller calculation was restricted to the high-symmetry axes, Γ → (π, 0) → (π, π) → Γ.
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    • R. S. Markiewicz, S. Sahrakorpi, M. Lindroos, Hsin Lin, and A. Bansil, Phys. Rev. B 72, 054519 (2005). In Fig. we introduce an effective t e f f ′ = t ′ - t ′, which controls the energy of the Van Hove singularity. 10.1103/PhysRevB.72.054519
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    • Markiewicz, R.S.1    Sahrakorpi, S.2    Lindroos, M.3    Lin, H.4    Bansil, A.5
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    • - is not expected to vary greatly with doping (Ref.)
    • - is not expected to vary greatly with doping (Ref.).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.