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Volumn 80, Issue 16, 2009, Pages

Exact ground states and correlation functions of chain and ladder models of interacting hardcore bosons or spinless fermions

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EID: 72449122949     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.80.165124     Document Type: Article
Times cited : (16)

References (39)
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    • A similar mapping is possible in the case of periodic boundary conditions, as has been discussed in Ref.; this is pertinent to the detailed analysis of exact diagonalizations as applied in Ref.. A significant complication of that case is that the mapping is no longer one-to-one. Instead, the mapping relates Bloch states constructed as linear combinations of configurations related by translation symmetry. The effective length for periodic boundary conditions is L′ =L-P.
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    • As we expect from having two flavors of bound pairs, the many-bound-pair ground state is twofold degenerate for ladders of even length L subject to periodic boundary conditions. For ladders of odd length L subject to periodic boundary conditions, the flavor of a bound pair changes as it goes around the boundary of the ladder, and so the conserved quantum numbers are not the even and odd flavors but are instead the symmetric and antisymmetric combinations of the two flavors. This mixing between even and odd flavors lifts the ground-state degeneracy giving a nondegenerate many-bound-pair ground state whose quantum number is the antisymmetric combination of flavors. In this paper we consider only ladders of even length L because we want to work with ground states containing bound pairs with a definite flavor.
    • As we expect from having two flavors of bound pairs, the many-bound-pair ground state is twofold degenerate for ladders of even length L subject to periodic boundary conditions. For ladders of odd length L subject to periodic boundary conditions, the flavor of a bound pair changes as it goes around the boundary of the ladder, and so the conserved quantum numbers are not the even and odd flavors but are instead the symmetric and antisymmetric combinations of the two flavors. This mixing between even and odd flavors lifts the ground-state degeneracy giving a nondegenerate many-bound-pair ground state whose quantum number is the antisymmetric combination of flavors. In this paper we consider only ladders of even length L because we want to work with ground states containing bound pairs with a definite flavor.
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    • More quantitatively, every sector maps to an ordinary fermion chain such that each change in flavor (between successive pairs) diminishes the effective length L′ by 1, thereby increasing the particle density (and hence the energy of that sector's ground state).
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    • The symmetry breaking has consequences for exact diagonalizations (Ref.). Since we always have the same number of spinless fermions on the two legs in this paired limit, we expect reflection about the ladder axis to be an exact symmetry of the ground states as well, as soon as | t/t′ | > 0 which permits a tiny tunnel amplitude between the even and odd sectors in finite ladders. The symmetrized ground states are 1 2 (| Ψ+ □ ± | Ψ- □).
    • The symmetry breaking has consequences for exact diagonalizations (Ref.). Since we always have the same number of spinless fermions on the two legs in this paired limit, we expect reflection about the ladder axis to be an exact symmetry of the ground states as well, as soon as | t/t′ | > 0 which permits a tiny tunnel amplitude between the even and odd sectors in finite ladders. The symmetrized ground states are 1 2 (| Ψ+ □ ± | Ψ- □).
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    • The CDW-π correlations □ Bj† Bj B j+r † Bj+r □ cannot be written as simple linear combinations of eight-point functions because a term like □ c 2,j † c 1,j+1 † c1,j+1 c2,j c 2,j+r+1 † c 1,j+r † c1,j+r c2,j+r+1 □ will pick up contributions from configurations that □ Bj† Bj B j+r † Bj+r □ will not. This tells us that □ Bj† Bj B j+r † Bj+r □ is some messy linear combination of 8-point, 12-point, 16-point,..., 4n -point functions.
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