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The Stability of Gapped Quantum Matter and Error-Correction with Adiabatic Noise

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arxiv 2402.14906 v1 pith:JT4RNRS4 submitted 2024-02-22 cond-mat.str-el cond-mat.stat-mechquant-ph

classification cond-mat.str-elcond-mat.stat-mechquant-ph
keywords quantumadiabaticphasecodenoiseerror-correctinggappedargue
verification ladder T0 review T1 audit T2 compute T3 formal
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The codespace of a quantum error-correcting code can often be identified with the degenerate ground-space within a gapped phase of quantum matter. We argue that the stability of such a phase is directly related to a set of coherent error processes against which this quantum error-correcting code (QECC) is robust: such a quantum code can recover from adiabatic noise channels, corresponding to random adiabatic drift of code states through the phase, with asymptotically perfect fidelity in the thermodynamic limit, as long as this adiabatic evolution keeps states sufficiently "close" to the initial ground-space. We further argue that when specific decoders -- such as minimum-weight perfect matching -- are applied to recover this information, an error-correcting threshold is generically encountered within the gapped phase. In cases where the adiabatic evolution is known, we explicitly show examples in which quantum information can be recovered by using stabilizer measurements and Pauli feedback, even up to a phase boundary, though the resulting decoding transitions are in different universality classes from the optimal decoding transitions in the presence of incoherent Pauli noise. This provides examples where non-local, coherent noise effectively decoheres in the presence of syndrome measurements in a stabilizer QECC.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Dissipative Dynamical Phase Transition as a Complex Ising Model

    quant-ph 2024-12 accept novelty 6.0 of 10

    The decay of a global spin-string observable in a dissipative qubit chain is exactly described by a complex-field Ising model, yielding a transition that is first-order-like from one side and second-order-like from the other.

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