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This study investigates the phase diagram of interacting Fibonacci anyons on a two-leg ladder, revealing distinct metallic and insulating regimes driven by repulsive interactions. By deriving an effective one-dimensional model via superexchange processes, researchers identify four specific phases including ferro- and antiferromagnetic golden chain states alongside exotic correlation patterns. These findings advance our theoretical understanding of topological order in strongly correlated quantum systems relevant to future fault-tolerant computing architectures.
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Phases of Interacting Fibonacci Anyons on a Ladder at Half-Filling

arXiv2 min read

arXiv:2507.22115v2 Announce Type: replace-cross Abstract: Two-dimensional many-body quantum systems can exhibit topological order and support collective excitations with anyonic statistics different from the usual fermionic or bosonic ones. With the emergence of these exotic point-like particles, it is natural to ask what phases can arise in interacting many-anyon systems. To study this topic, we consider the particular case of Fibonacci anyons subject to an anyonic tight-binding model with nearest-neighbor repulsion on a two-leg ladder. Focusing on the case of half-filling, for low interaction strengths an ``anyonic'' metal is found, whereas for strong repulsion, the anyons form an insulating charge-density wave. Within the latter regime, we introduce an effective one-dimensional model up to sixth order in perturbation theory arising from anyonic superexchange processes. We numerically identify four distinct phases of the effective model, which we characterize using matrix product state methods. These include both the ferro- and antiferromagnetic golden chain phases, as well as phases with $\mathbb{Z}_2$ and incommensurate correlations.

Abstract:Two-dimensional many-body quantum systems can exhibit topological order and support collective excitations with anyonic statistics different from the usual fermionic or bosonic ones. With the emergence of these exotic point-like particles, it is natural to ask what phases can arise in interacting many-anyon systems. To study this topic, we consider the particular case of Fibonacci anyons subject to an anyonic tight-binding model with nearest-neighbor repulsion on a two-leg ladder. Focusing on the case of half-filling, for low interaction strengths an ``anyonic'' metal is found, whereas for strong repulsion, the anyons form an insulating charge-density wave. Within the latter regime, we introduce an effective one-dimensional model up to sixth order in perturbation theory arising from anyonic superexchange processes. We numerically identify four distinct phases of the effective model, which we characterize using matrix product state methods. These include both the ferro- and antiferromagnetic golden chain phases, as well as phases with $\mathbb{Z}_2$ and incommensurate correlations.

Strongly Correlated Electrons (cond-mat.str-el); Quantum Physics (quant-ph)

arXiv:2507.22115 [cond-mat.str-el]

(or arXiv:2507.22115v2 [cond-mat.str-el] for this version)

https://doi.org/10.48550/arXiv.2507.22115 Focus to learn more arXiv-issued DOI via DataCite

Phys. Rev. B 114, 045117 (2026)

https://doi.org/10.1103/c92g-mhly Focus to learn more DOI(s) linking to related resources

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Full text under the publisher's open licence · 266 words

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