2006
DOI: 10.1103/physrevb.73.045125
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Renormalization-group analysis of the one-dimensional extended Hubbard model with a single impurity

Abstract: We analyze the one-dimensional extended Hubbard model with a single static impurity by using a computational technique based on the functional renormalization group. This extends previous work for spinless fermions to spin-1 2 fermions. The underlying approximations are devised for weak interactions and arbitrary impurity strengths, and have been checked by comparing with density matrix renormalization group data. We present results for the density of states, the density profile and the linear conductance. Two… Show more

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Cited by 46 publications
(75 citation statements)
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“…In the presence of a sizable backscattering component (g 1,⊥ > 0) the asymptotic low-energy regime is usually reached via a complex crossover behavior [6,7,8]. We expect the same to hold for the more realistic setups studied here, which would render the behavior of G(T ) even more complex (and less "universal") than described in the present work.…”
Section: Introductionsupporting
confidence: 56%
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“…In the presence of a sizable backscattering component (g 1,⊥ > 0) the asymptotic low-energy regime is usually reached via a complex crossover behavior [6,7,8]. We expect the same to hold for the more realistic setups studied here, which would render the behavior of G(T ) even more complex (and less "universal") than described in the present work.…”
Section: Introductionsupporting
confidence: 56%
“…General aspects of the fRG can be found in [23], [24], and [25], while its application to inhomogeneous LLs is described in [8], [11] and [16]. By comparison to results for small systems obtained by density-matrix renormalization group and to exact results from bosonization and Bethe ansatz for the asymptotic behavior, it was shown that the fRG in the truncation scheme used here captures the relevant physics not only in the asymptotic low-energy regime but also on finite energy scales [11,16].…”
Section: The Functional Renormalization Groupmentioning
confidence: 99%
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“…This can be understood as follows. The crossover scale ∆ is strongly affected by the size of the open boundary analog of a g 1,⊥ two-particle scattering process [17,36,40] which cannot be written quadratically in the bosonic densities. Its initial value (with respect to an RG flow) in the extended Hubbard model is given by g 1,⊥ = U + 2V cos(2k F ) with k F = nπ/2.…”
Section: Spectral Properties Of the Extended Hubbard Modelmentioning
confidence: 99%
“…For the extended Hubbard model and vanishing SOI, this has been done in Ref. 16 using fRG. As the parameterization of the two-particle vertex used there relies on spin conservation, it cannot easily be extended to the present situation with SOI.…”
Section: 16mentioning
confidence: 99%