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Disorder as an Ally: Quantum Memory ⚡ экспресс

Original: "Emergent Decoherence Dynamics in Doubly Disordered Spin Networks"
arXiv:2511.07785 · 2025-11-11 · CC BY 4.0 · ⏱ 1 min · Quantum Physics Mesoscale
Physicists have discovered that disorder can protect quantum information, not destroy it.
Abstract

In a doubly disordered network of electronic and nuclear spins, a universal decoherence law of nuclear polarization has been discovered, characterized by two-stage decay: an initial fast exponential drop followed by a slow decay described by a stretched exponential with an exponent of 1/2. Microscopically, it originates from two interrelated channels: long-range interaction via the electronic network and anomalous subdiffusive transport in the nuclear subsystem. The possibility of selective control or elimination of each channel via Floquet engineering and optical modulation of the environment has been demonstrated. Contrary to expectations, disorder plays a protective role, forming isolated electron-free clusters that localize polarization and prolong coherence time. These results provide a microscopic basis for managing decoherence pathways and propose engineered disorder as a new design principle for long-lived quantum memories and sensors.

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In everyday life, order saves, disorder destroys. With quantum information, it's the opposite. In diamond, electrons and carbon nuclei act like tiny magnets storing a whisper. Gossipy electrons spread it instantly; nuclei pass it along the chain slowly. But crystal imperfections create quiet dead ends where leakage can't enter—there the whisper lives hundreds of times longer.

Decay law: e^{-√(R_p t)} e^{-R_d t}. R_p is the strength of long-range magnetic couplings, R_d is the nuclear mixing rate.

With light pulses (optical spectroscopy), we can hush the gossip or slow the chain. The growth of entropy, the measure of chaos, usually destroys order. Yet local disorder blocks global decay. This was already pondered by Schrödinger and von Neumann. Conclusion: long-lived quantum memory requires not sterile purity but a dose of chaos.

🎯 At room temperature, such quantum states decay in milliseconds, but in the described experiment, the lifetime grew hundreds of times longer thanks to isolated 'pockets' in the crystal.

e^{-\sqrt{R_p t}} e^{-R_d t}
The probability that the quantum state does not decay after time t. R_p accounts for long-range magnetic couplings, R_d for slow mixing of nuclear states.
Scientists
Christian DopplerD. B. McLaughlinDidier QuelozMichel MayorR. A. RossiterJacob Bekenstein
Tags
entropy carbon spectroscopy
Laws
second law of thermodynamicsDoppler effectBekenstein-Hawking entropyMaxwell's equationsPlanck's lawPlanck–Einstein relation
Original: arXiv:2511.07785 · CC BY 4.0 · bridge42worlds