(37) This equation must be interpreted as a Stratonovich stochastic differential equation, where ˙θ and ˜µq(θ(t), t) are not independent

In this new basis, the resulting stochastic master equation for ˜µq(t) ≡ ˜µq(θ(t), t) reads ˙˜µq(t) = [L0 + r0 (L+ + L−)] ˜µq(t) − i ˙θ 2[Sz, ˜µq(t)]

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quant-ph · 2025-06-25 · unverdicted · novelty 6.0

Non-Markovian thermal reservoirs generate stationary entanglement between distant qubits via a quasiadiabatic dark state.

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Non-Markovian thermal reservoirs for autonomous entanglement distribution quant-ph · 2025-06-25 · unverdicted · none · ref 1
Non-Markovian thermal reservoirs generate stationary entanglement between distant qubits via a quasiadiabatic dark state.