Fractional quantum Hall states under density decoherence

• URL: http://arxiv.org/abs/2510.08490v1
• Date: Thu, 09 Oct 2025 17:30:37 GMT
• Title: Fractional quantum Hall states under density decoherence
• Abstract summary: We investigate how the information encoded in two paradigmatic states, the Laughlin and Moore-Read states, is affected by density decoherence.<n>For Laughlin states, information encoded in the topological ground state manifold degrades continuously with decoherence strength inside this critical phase.<n>On the other hand, quantum information encoded in the fusion space of non-abelian anyons of the Moore-Read states remains fully recoverable for arbitrary strong decoherence.
• Score: 2.91406628418801
• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Fractional quantum Hall states are promising platforms for topological quantum computation due to their capacity to encode quantum information in topologically degenerate ground states and in the fusion space of non-abelian anyons. We investigate how the information encoded in two paradigmatic states, the Laughlin and Moore-Read states, is affected by density decoherence -- coupling of local charge density to non-thermal noise. We identify a critical filling factor $\nu_c$, above which the quantum information remains fully recoverable for arbitrarily strong decoherence. The $\nu=1/3$ Laughlin state and $\nu = 1/2$ Moore-Read state both lie within this range. Below $\nu_c$ both classes of states undergo a decoherence induced Berezinskii-Kosterlitz-Thousless (BKT) transition into a critical decohered phase. For Laughlin states, information encoded in the topological ground state manifold degrades continuously with decoherence strength inside this critical phase, vanishing only in the limit of infinite decoherence strength. On the other hand, quantum information encoded in the fusion space of non-abelian anyons of the Moore-Read states remains fully recoverable for arbitrary strong decoherence even beyond the BKT transition. These results lend further support to the promise of non-Abelian FQH states as platforms for topological quantum computation and raises the question of how errors in such states can be corrected.

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