2018
DOI: 10.1103/physrevb.97.235126
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Detecting phases in one-dimensional many-fermion systems with the functional renormalization group

Abstract: The functional renormalization group (FRG) has been used widely to investigate phase diagrams, in particular the one of the two-dimensional Hubbard model. So far, the study of one-dimensional models has not attracted as much attention. We use the FRG to investigate the phases of a onedimensional spinless tight-binding chain with nearest and next-nearest neighbor interactions at half filling. The phase diagram of this model has already been established with other methods, and phase transitions from a metallic p… Show more

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Cited by 27 publications
(32 citation statements)
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“…In contrast to both mean-field and perturbation theory, our RG approach yields a finite value of U crit in the limit Γ ¼ E ¼ 0 in accord with the analytic solution [36]. Moreover, we quantitatively reproduce an exact result for the phase boundary at Γ > 0 in the limit U → ∞.…”
supporting
confidence: 61%
See 1 more Smart Citation
“…In contrast to both mean-field and perturbation theory, our RG approach yields a finite value of U crit in the limit Γ ¼ E ¼ 0 in accord with the analytic solution [36]. Moreover, we quantitatively reproduce an exact result for the phase boundary at Γ > 0 in the limit U → ∞.…”
supporting
confidence: 61%
“…Phase diagram.-To probe spontaneous symmetry breaking and the transition into a CDW phase, we add a small staggered on site potential s to the Hamiltonian [36] and compute the susceptibility…”
mentioning
confidence: 99%
“…In this work, we aim to account for all second-order terms. This has so far only been achieved in thermal equilibrium [21][22][23][24][25] as well as for the singleimpurity Anderson model out of equilibrium [26].…”
Section: Second-order Frg Formulationmentioning
confidence: 99%
“…In contrast to previous approaches to this problem [17], we incorporate second-order contributions and can therefore describe inelastic processes and heating effects. Due to the significant numerical cost, second-order FRG schemes have so far only been implemented for electronic systems in thermal equilibrium [21][22][23][24][25] as well as for the single-impurity Anderson model out of equilibrium [26].…”
Section: Introductionmentioning
confidence: 99%
“…The particles are subject to a repulsive interaction on nearest-and nextnearest-neighbor sites, which we fix to U = 1 and U = 0.5 so as to model a lattice analog of the Coulomb interaction. This parameter choice places the system in a metallic, but strongly correlated phase in absence of a potential V i , even at half filling [39].…”
Section: Modelmentioning
confidence: 99%