2012
DOI: 10.1103/physrevb.86.121105
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Sublattice interference in the kagome Hubbard model

Abstract: We study the electronic phases of the kagome Hubbard model (KHM) in the weak-coupling limit around Van Hove filling. Through an analytic renormalization group analysis, we find that there exists a sublattice interference mechanism where the kagome sublattice structure affects the character of the Fermi surface instabilities. It leads to major suppression of T c for d + id superconductivity in the KHM and causes an anomalous increase of T c upon addition of longer-range Hubbard interactions. We conjecture that … Show more

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Cited by 207 publications
(203 citation statements)
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“…Our results are also relevant for interacting electron systems without preformed local moments, such as Hubbard-type models [36][37][38][39]. The kagome tight-binding model is expected to exhibit weak-coupling instabilities when the electron filling reaches the QBCP or the Van Hove singularities.…”
Section: Introductionmentioning
confidence: 85%
“…Our results are also relevant for interacting electron systems without preformed local moments, such as Hubbard-type models [36][37][38][39]. The kagome tight-binding model is expected to exhibit weak-coupling instabilities when the electron filling reaches the QBCP or the Van Hove singularities.…”
Section: Introductionmentioning
confidence: 85%
“…Either way, the computational effort of fRG studies may be lowered considerably, in particular for two-dimensional systems with a sixfold symmetry, such as multilayer graphene [5][6][7] and electrons on a Kagome lattice [15,19]. Currently, two of us are preparing a publication on an fRG study of the Emery model with non-zero oxygen-oxygen hopping and at weak coupling.…”
Section: Discussionmentioning
confidence: 99%
“…An on-site Hubbard term, for example, is then rendered nonlocal by this so-called orbital makeup [25], which may have a considerable impact on the phase diagram of multiband models for unconventional superconductors, for example. It is also believed to account for the differences between the phase diagrams of extended Hubbard models on the honeycomb and the Kagome lattices [15,19]. In addition, it lends a non-trivial behavior under point-group operations to the interaction.…”
Section: Hybridizing and Non-hybridizing Bloch Basesmentioning
confidence: 99%
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