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arxiv: 1005.1604 · v1 · pith:Z6WHUPPRnew · submitted 2010-05-10 · 🪐 quant-ph · cond-mat.stat-mech

Nakajima-Zwanzig versus time-convolutionless master equation for the non-Markovian dynamics of a two-level system

classification 🪐 quant-ph cond-mat.stat-mech
keywords nakajima-zwanzigtime-convolutionlessequationexactmastersystemcontributiondifferent
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We consider the exact reduced dynamics of a two-level system coupled to a bosonic reservoir, further obtaining the exact time-convolutionless and Nakajima-Zwanzig non-Markovian equations of motion. The considered system includes the damped and undamped Jaynes-Cummings model. The result is obtained by exploiting an expression of quantum maps in terms of matrices and a simple relation between the time evolution map and time-convolutionless generator as well as Nakajima-Zwanzig memory kernel. This non-perturbative treatment shows that each operator contribution in Lindblad form appearing in the exact time-convolutionless master equation is multiplied by a different time dependent function. Similarly, in the Nakajima-Zwanzig master equation each such contribution is convoluted with a different memory kernel. It appears that depending on the state of the environment the operator structures of the two set of equations of motion can exhibit important differences.

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    New proof via Lyapunov exponents that the largest decay rate Γ_max in a d-dimensional quantum master equation satisfies Γ_max ≤ κ_d times the sum of the other d²-1 decay rates, with κ_d depending only on d and the map class.