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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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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.
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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.
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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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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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27
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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- □).
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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- □).
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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.
-
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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Technically, the correct thing to do is to compute the p -particle sector of the cluster density matrix of a (p+1) -site cluster and look at the matrix element between a configuration with an empty site at the left end of the cluster and a configuration with an empty site at the right end of the cluster. However, the relevant cluster density matrix is that of a system of hardcore bosons. While this hardcore-boson cluster density matrix should be simply related to the noninteracting-spinless-fermion cluster density matrix, this relation has not been worked out for use on this problem of finding FL correlations at large r for the bound-pair ground states on a two-legged ladder.
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Technically, the correct thing to do is to compute the p -particle sector of the cluster density matrix of a (p+1) -site cluster and look at the matrix element between a configuration with an empty site at the left end of the cluster and a configuration with an empty site at the right end of the cluster. However, the relevant cluster density matrix is that of a system of hardcore bosons. While this hardcore-boson cluster density matrix should be simply related to the noninteracting-spinless-fermion cluster density matrix, this relation has not been worked out for use on this problem of finding FL correlations at large r for the bound-pair ground states on a two-legged ladder.
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Whenever we explicitly discuss ground states, e.g., in studies of exact diagonalization (Ref.), it is appropriate to make the ground states symmetric or antisymmetric under reflection about the ladder axis, namely, | Ψ ± □ = (| Ψ 1 □ ± | Ψ 2 □)/2. If | t□ /t | > 0, the sectors become connected with a tiny tunnel amplitude in a finite system; in this case only the symmetry-restored states | Ψ± □ are actual eigenstates.
-
Whenever we explicitly discuss ground states, e.g., in studies of exact diagonalization (Ref.), it is appropriate to make the ground states symmetric or antisymmetric under reflection about the ladder axis, namely, | Ψ± □ = (| Ψ1 □ ± | Ψ2 □)/2. If | t □ /t | >0, the sectors become connected with a tiny tunnel amplitude in a finite system; in this case only the symmetry-restored states | Ψ± □ are actual eigenstates.
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