2020
DOI: 10.1103/physrevresearch.2.033267
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Interaction-induced topological properties of two bosons in flat-band systems

Abstract: In flat-band systems, destructive interference leads to the localization of noninteracting particles and forbids their motion through the lattice. However, in the presence of interactions the overlap between neighboring single-particle localized eigenstates may enable the propagation of bound pairs of particles. In this work, we show how these interaction-induced hoppings can be tuned to obtain a variety of two-body topological states. In particular, we consider two interacting bosons loaded into the orbital a… Show more

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Cited by 38 publications
(16 citation statements)
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“…. Diagonalization of the Hamiltonian in ( 1) yields an all-bands flat energy spectrum 18 , shown in Fig. 1(c), as a consequence of an Aharonov-Bohm caging effect induced by the π-flux in each plaquette [19][20][21] .…”
Section: Diamond Chain With π-Flux Per Plaquettementioning
confidence: 99%
See 1 more Smart Citation
“…. Diagonalization of the Hamiltonian in ( 1) yields an all-bands flat energy spectrum 18 , shown in Fig. 1(c), as a consequence of an Aharonov-Bohm caging effect induced by the π-flux in each plaquette [19][20][21] .…”
Section: Diamond Chain With π-Flux Per Plaquettementioning
confidence: 99%
“…The first term in ( 4) is quantized to either 0 or π such that, modulo 2π, one necessarily has γ ± = π 2 . The states of the zero-energy flat band n = 0, on the other hand, have no weight on the A sublattice 18 , so the usual π-quantization holds for γ 0 .…”
Section: Diamond Chain With π-Flux Per Plaquettementioning
confidence: 99%
“…The physics of two-body bound states in the presence of a flat band has been recently explored theoretically in different contexts, including topological matter [17][18][19][20] and the link between the inverse effective mass of the bound state and the quantum metric of the singleparticle states [21][22][23]. This second direction is related to the more general question of understanding how transport and superconductivity can occur in system with quenched kinetic energy [24][25][26][27][28][29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, as the first step towards understanding topological many-body systems, one may judiciously focus on the simplest nontrivial subspace with interactions, that of only two excitations. Indeed, the two-excitation sector already provides some hallmarks of multi-excitation physics, such as bound two-particle states and novel bands in the quasiparticle bandstructure [20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%