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By expanding |C1⟩, which is the vectorized form of the first block of the local steady state, in powers of g |C1⟩ = ∞∑ n=0 gn ⏐ ⏐ ⏐C(n) ⟩ , (C3) and using Eq

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quant-ph 1

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2025 1

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An open harmonic chain: Exact vs global and local reduced dynamics

quant-ph · 2025-05-22 · conditional · novelty 5.0

For a three-oscillator chain with two unequal-temperature baths, the local GKSL master equation is numerically closer to the exact dynamics for weak inter-oscillator coupling, while the global equation wins above a temperature-dependent critical coupling.

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  • An open harmonic chain: Exact vs global and local reduced dynamics quant-ph · 2025-05-22 · conditional · none · ref 3

    For a three-oscillator chain with two unequal-temperature baths, the local GKSL master equation is numerically closer to the exact dynamics for weak inter-oscillator coupling, while the global equation wins above a temperature-dependent critical coupling.