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This study identifies a specific, transferable operating regime for dissipative quantum reservoir computing where performance remains robust across tasks and hardware configurations. By mapping the interplay between input drive strength, qubit coupling, and dissipation rates, researchers define a "memory-defined" region that can be efficiently located using simple diagnostics before deployment. The findings provide actionable guidance for leveraging current noisy intermediate-scale quantum (NISQ) devices without optimizing complex internal dynamics.
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Where a Quantum Reservoir Works: A Transferable Operating Band

arXiv2 min de cititArticolul și perspectiva sunt în engleză.

arXiv:2606.13284v1 Announce Type: new Abstract: In quantum reservoir computing, a fixed quantum system transforms an input signal, while learning reduces to training a simple linear readout on its measured outputs. Since the quantum dynamics themselves are never optimized, the method is well suited to today's hardware. Yet these dynamics must still be chosen carefully, because their settings remain fixed throughout training and inference. It therefore remains an open question where, in its control space, a fixed quantum system learns well. We address this question for a dissipative reservoir by mapping performance over three central physical controls: the strength of the input drive, the coupling between neighboring qubits, and the rate of dissipation. Good performance concentrates in a single, well-defined operating region of this control space. This region transfers across tasks and reservoir initializations, and the same memory-defined regime persists under architectural changes. It is also mechanistically grounded, since it disappears whenever any of the mechanisms that create it is removed. Finally, the region can be located cheaply before any task is run, using a simple memory diagnostic.

Abstract:In quantum reservoir computing, a fixed quantum system transforms an input signal, while learning reduces to training a simple linear readout on its measured outputs. Since the quantum dynamics themselves are never optimized, the method is well suited to today's hardware. Yet these dynamics must still be chosen carefully, because their settings remain fixed throughout training and inference. It therefore remains an open question where, in its control space, a fixed quantum system learns well. We address this question for a dissipative reservoir by mapping performance over three central physical controls: the strength of the input drive, the coupling between neighboring qubits, and the rate of dissipation. Good performance concentrates in a single, well-defined operating region of this control space. This region transfers across tasks and reservoir initializations, and the same memory-defined regime persists under architectural changes. It is also mechanistically grounded, since it disappears whenever any of the mechanisms that create it is removed. Finally, the region can be located cheaply before any task is run, using a simple memory diagnostic.

arXiv:2606.13284 [quant-ph]

(or arXiv:2606.13284v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2606.13284 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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