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cos Ωt − 2XtX0] + g sin Ωt tZ 0 dsxk(s){Xt sin Ωs + X0 sin[Ω(t − s)]} (6) − g2 MΩ sin Ωt tZ 0 ds sZ 0 du sin Ωu sin[Ω(t − s)]xk(u)xk(s)

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quant-ph 1

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2025 1

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UNVERDICTED 1

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Objectivity in the quantum Brownian motion revisited

quant-ph · 2025-06-17 · unverdicted · novelty 5.0

Objectivity in finite-environment quantum Brownian motion holds only on timescales defined by oscillator frequency ratios and is enhanced near phase π/2 due to trajectory effects.

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  • Objectivity in the quantum Brownian motion revisited quant-ph · 2025-06-17 · unverdicted · none · ref 1

    Objectivity in finite-environment quantum Brownian motion holds only on timescales defined by oscillator frequency ratios and is enhanced near phase π/2 due to trajectory effects.