The Lindblad master equation decomposes into free evolution plus generalized charge exchange plus dephasing, unifying strong-coupling, particle-exchange, and non-Abelian effects under one physical structure.
To this end, we choose: A3 = 1 2i[A1;A 2] (B3) orthogonal to bothA 1 andA 2
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Revealing the physical structure of the general quantum master equation
The Lindblad master equation decomposes into free evolution plus generalized charge exchange plus dephasing, unifying strong-coupling, particle-exchange, and non-Abelian effects under one physical structure.