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An example of such a strong-coupling liquid is the quantum Heisenberg paramagnet at a sufficiently high temperature. It has translation invariance and rotation invariance intact but has no simple adiabatic relationship to a free gas with the same symmetries. The ECQL takes such a spin liquid and further introduces mobile charges into it.
-
An example of such a strong-coupling liquid is the quantum Heisenberg paramagnet at a sufficiently high temperature. It has translation invariance and rotation invariance intact but has no simple adiabatic relationship to a free gas with the same symmetries. The ECQL takes such a spin liquid and further introduces mobile charges into it.
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77954830315
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In common with standard many-body theory (Refs.), the Green's function is expressed in terms of a self-energy, the self-energy in terms of a vertex function, and the vertex function satisfies integral equations involving various susceptibilities and also higher-order vertices.
-
In common with standard many-body theory (Refs.), the Green's function is expressed in terms of a self-energy, the self-energy in terms of a vertex function, and the vertex function satisfies integral equations involving various susceptibilities and also higher-order vertices.
-
-
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32
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77954832428
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-
In standard perturbation theory, e.g., as discussed in Refs., an expansion in bare Green's functions is resummed to give the skeleton graph expansion for the self-energy Σ, or compact diagrams for the grand potential Ω, where the internal lines are all the full Green's function. The Schwinger source technique quite naturally generates a series that is completely analogous to this skeleton graph expansion and bypasses the first stage of bare lines. In this sense, the lack of Wick's theorem for the Hubbard operators that prevents a regular Feynman-type analysis, is overcome by employing the Schwinger approach.
-
In standard perturbation theory, e.g., as discussed in Refs., an expansion in bare Green's functions is resummed to give the skeleton graph expansion for the self-energy Σ, or compact diagrams for the grand potential Ω, where the internal lines are all the full Green's function. The Schwinger source technique quite naturally generates a series that is completely analogous to this skeleton graph expansion and bypasses the first stage of bare lines. In this sense, the lack of Wick's theorem for the Hubbard operators that prevents a regular Feynman-type analysis, is overcome by employing the Schwinger approach.
-
-
-
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33
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77954822102
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-
It is important to verify that the self-energy and vertices are well behaved at high frequencies ω (i.e., have the form ∼ c1 + c2 ω), and possess proper spectral representations. When these conditions are not satisfied, as with equations formally following from those of G without the removal of the factor of Δ as in Eq. , we denote the resulting equations as ill formed.
-
It is important to verify that the self-energy and vertices are well behaved at high frequencies ω (i.e., have the form ∼ c 1 + c 2 ω), and possess proper spectral representations. When these conditions are not satisfied, as with equations formally following from those of G without the removal of the factor of Δ as in Eq., we denote the resulting equations as ill formed.
-
-
-
-
34
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77954828694
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-
note
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- 1 [i, f]. We can then convert the asymmetric Γ vertices to the symmetric vertices Λ using this prescription.
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-
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35
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77954834007
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-
This represents the dynamical inverse and should not to be confused with a matrix inverse.
-
This represents the dynamical inverse and should not to be confused with a matrix inverse.
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36
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33847686755
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Y. Takahashi, Nuovo Cimento 10, 370 (1957). Takahashi's relativistic version of the conservation law is easily generalized as here for a discrete hopping problem with arbitrary band structure.
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Takahashi, Y.1
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46
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77954833754
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On the other hand, for the Hubbard model, it is easy to show that the triplet vertices satisfy finite versions of the Ward identity analogous to Eqs. , since the spin density commutes with the interaction terms.
-
On the other hand, for the Hubbard model, it is easy to show that the triplet vertices satisfy finite versions of the Ward identity analogous to Eqs., since the spin density commutes with the interaction terms.
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47
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(unpublished).
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77954823330
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The Hubbard-I solution (Ref.) of the finite- U version has been criticized in literature (Ref.), for failing to reproduce the Luttinger volume theorem even in the U→0 limit. We see here that while it remains incorrect for all finite values of U, it does give the correct renormalized volume at U→
-
The Hubbard-I solution (Ref.) of the finite- U version has been criticized in literature (Ref.), for failing to reproduce the Luttinger volume theorem even in the U → 0 limit. We see here that while it remains incorrect for all finite values of U, it does give the correct renormalized volume at U →
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A. J. Leggett, Rev. Mod. Phys. 47, 331 (1975). Leggett's recommendation of using a pseudopotential (page 344 footnote 6) is valuable in our context. 10.1103/RevModPhys.47.331
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57
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77954826769
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The extended s -wave channel is also excluded by force in our projections and so this treatment does not give a fair chance to that specific order.
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The extended s -wave channel is also excluded by force in our projections and so this treatment does not give a fair chance to that specific order.
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exact diagonalizations computing the FS volume in, 10.1103/PhysRevB.75. 045111
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77954832639
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-
At the time of completing the mansuscript, we noticed papers on the t-J model, Ref., with some initial overlap with our method. We differ in much of the details and the conclusions. These authors consider only density (but not spin)-dependent sources, and thus do not obtain the analogs of most of our main results, e.g., the exact Schwinger Dyson equation, Eq. . They further make what seem to be uncontrolled approximations, leading to results that are in disagreement with ours. For instance, they find an effective band that vanishes as (1-n ) near half filling, in contrast to our reduction in the bandwidth by spin and density correlations.
-
At the time of completing the mansuscript, we noticed papers on the t - J model, Ref., with some initial overlap with our method. We differ in much of the details and the conclusions. These authors consider only density (but not spin)-dependent sources, and thus do not obtain the analogs of most of our main results, e.g., the exact Schwinger Dyson equation, Eq.. They further make what seem to be uncontrolled approximations, leading to results that are in disagreement with ours. For instance, they find an effective band that vanishes as (1 - n) near half filling, in contrast to our reduction in the bandwidth by spin and density correlations.
-
-
-
-
69
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77954832157
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-
has brought to my attention a recent preprint:, arXiv:0909.3069 (unpublished), where charge 2e objects arise dynamically in the Hubbard model.
-
Prof. P. Phillips has brought to my attention a recent preprint: S. Chakraborty, S. Hong, and P. Phillips, arXiv:0909.3069 (unpublished), where charge 2 e objects arise dynamically in the Hubbard model.
-
-
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Phillips, P.1
Chakraborty, S.2
Hong, S.3
Phillips, P.4
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70
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77954824133
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-
Its functional derivatives w.r.t. the sources also seems negligible at first sight but we plan to check this more carefully later. For now it must be taken as an assumption for the vertex that is certainly consistent with the Ward identity.
-
Its functional derivatives w.r.t. the sources also seems negligible at first sight but we plan to check this more carefully later. For now it must be taken as an assumption for the vertex that is certainly consistent with the Ward identity.
-
-
-
-
71
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77954821490
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-
This analysis parallels that of Sec. 6.1 for the Bethe Salpeter equations for particle-hole multiple scattering (Ref.).
-
This analysis parallels that of Sec. 6.1 for the Bethe Salpeter equations for particle-hole multiple scattering (Ref.).
-
-
-
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72
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77954823189
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There is another way to group particles and holes leading to a second particle-hole channel familiar in parquet theory but we will choose this present one since it is most relevant.
-
There is another way to group particles and holes leading to a second particle-hole channel familiar in parquet theory but we will choose this present one since it is most relevant.
-
-
-
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73
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77954829419
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The vertices obtained from this atomic Green's function and the "untreated" self-energy where the transformation, Eq. , has not been done, are easily seen to contain linear terms at high frequency and hence are examples of a "sick" theory.
-
The vertices obtained from this atomic Green's function and the "untreated" self-energy where the transformation, Eq., has not been done, are easily seen to contain linear terms at high frequency and hence are examples of a "sick" theory.
-
-
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74
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77954820408
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We have preliminary results showing how the singular part of the self-energy and the Luttinger-Ward functional arise from a partial summation of an infinite set of diagrams in perturbation theory of the Hubbard model.
-
We have preliminary results showing how the singular part of the self-energy and the Luttinger-Ward functional arise from a partial summation of an infinite set of diagrams in perturbation theory of the Hubbard model.
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