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Volumn 81, Issue 4, 2010, Pages

Erratum: Liquid crystal phases of ultracold dipolar fermions on a lattice (Phys. Rev. B (2010) 81 (045115) DOI: 10.1103/PhysRevB.81.045115);Liquid crystal phases of ultracold dipolar fermions on a lattice

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EID: 77954826315     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.83.119901     Document Type: Erratum
Times cited : (35)

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    • Strictly speaking the d -density wave is not a mean-field solution to the extended Hubbard model in the sense that one cannot obtain the value of order parameter from a set of self-consistency equations. However one could use the variational principle to argue that the d -density wave has lower energy than the isotropic state. To estimate the critical U of d -density wave, we first decompose the interaction into -1 N Σ k k ′ V k-k′) c k † c k + Q c k ′ † c k ′ - Q, identifying the coefficient V′ common to those in f (k ) f (k′ ) with f (k ) =cos kx -cos ky. We then approximate the interaction as V′ N Σk k′ f (k ) f (k′ ) c k † c k + Q c k′ † c k′ - Q, where d -density wave is naturally a mean-field solution. Note that by doing so, the so-called extended s -density wave [f (k ) =cos kx +cos ky ] has the same critical U as that of d -density wave.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.