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Volumn 68, Issue 6, 2003, Pages 24-

Spin-exchange interactions of spin-one bosons in optical lattices: Singlet, nematic, and dimerized phases

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EID: 80255134785     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.68.063602     Document Type: Article
Times cited : (81)

References (52)
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    • F. Zhou, e-print cond-mat/0108473 (unpublished)
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    • F. Zhoue-print cond-mat/0207041 (unpublished).
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    • P.G. de Gennes and J. Prost, The Physics of Liquid Crystals (Oxford Press, Oxford, 1993)
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    • Expression (42) describes an eigenstate of (Formula presented) with eigenvalue zero. After an SU(2) rotation we will have (Formula presented) that is an eigenstate of (Formula presented) with zero eigenvalue. Vector (Formula presented) corresponds to the direction of uniaxial nematic
    • Expression (42) describes an eigenstate of (Formula presented) with eigenvalue zero. After an SU(2) rotation we will have (Formula presented) that is an eigenstate of (Formula presented) with zero eigenvalue. Vector (Formula presented) corresponds to the direction of uniaxial nematic.
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    • M. Greiner, e-print cond-mat/0207196 (unpublished).
    • Greiner, M.1
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    • E. Demler, F. Zhou, and F.D.M. Haldane, Report No. ITP-UU-01/09, 2001
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    • The operator b applied directly to (Formula presented) takes us outside of the physical Hilbert space since it does not change the symmetry of the (Formula presented) wave function simultaneously with changing the number of particles by one. The physical Hamiltonian, however, will always have this operator b in combination with some odd function of (Formula presented) and will preserve the physical Hilbert space
    • The operator b applied directly to (Formula presented) takes us outside of the physical Hilbert space since it does not change the symmetry of the (Formula presented) wave function simultaneously with changing the number of particles by one. The physical Hamiltonian, however, will always have this operator b in combination with some odd function of (Formula presented) and will preserve the physical Hilbert space.
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    • J.W. Negele and H. Orland, Quantum Many-Particle Systems (Addison-Wesley, New York, 1988).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.