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Unifying non-Markovian characterisation with an efficient and self-consistent framework

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arxiv 2312.08454 v2 pith:HKQV6OTJ submitted 2023-12-13 quant-ph

classification quant-ph
keywords quantumdevicesframeworkcircuitcorrelationsdecouplingeffectsefficient
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abstract

Noise on quantum devices is much more complex than it is commonly given credit. Far from usual models of decoherence, nearly all quantum devices are plagued both by a continuum of environments and temporal instabilities. These induce noisy quantum and classical correlations at the level of the circuit. The relevant spatiotemporal effects are difficult enough to understand, let alone combat. There is presently a lack of either scalable or complete methods to address the phenomena responsible for scrambling and loss of quantum information. Here, we make deep strides to remedy this problem. We establish a theoretical framework that uniformly incorporates and classifies all non-Markovian phenomena. Our framework is universal, assumes no parameters values, and is written entirely in terms of experimentally accessible circuit-level quantities. We formulate an efficient reconstruction using tensor network learning, allowing also for easy modularisation and simplification based on the expected physics of the system. This is then demonstrated through both extensive numerical studies and implementations on IBM Quantum devices, estimating a comprehensive set of spacetime correlations. Finally, we conclude our analysis with applications thereof to the efficacy of control techniques to counteract these effects -- including noise-aware circuit compilation and optimised dynamical decoupling. We find significant improvements are possible in the diamond norm and average gate fidelity of arbitrary $SU(4)$ operations, as well as related decoupling improvements in contrast to off-the-shelf schemes.

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  1. Two-point measurement correlations beyond the quantum regression theorem

    quant-ph 2025-07 conditional novelty 7.0 of 10

    A generalized quantum regression formula holds exactly for processes with classical memory, and its violation is a detectable witness of quantum memory, with applications to the spin-boson model.

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