2013
DOI: 10.1590/s1806-11172013000100003
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A simple derivation of the Lindblad equation

Abstract: We present a derivation of the Lindblad equation - an important tool for the treatment of non-unitary evolutions - that is accessible to undergraduate students in physics or mathematics with a basic background on quantum mechanics. We consider a specific case, corresponding to a very simple situation, where a primary system interacts with a bath of harmonic oscillators at zero temperature, with an interaction Hamiltonian that resembles the Jaynes-Cummings format. We start with the Born-Markov equation and, tra… Show more

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Cited by 37 publications
(30 citation statements)
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References 9 publications
(7 reference statements)
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“…Refs. [47,[88][89][90][91], we pay special attention to the physical assumptions the Lindblad formalism relies on, and show how they concretely enter into the calculation.…”
Section: A Deriving the Lindblad Equationmentioning
confidence: 99%
“…Refs. [47,[88][89][90][91], we pay special attention to the physical assumptions the Lindblad formalism relies on, and show how they concretely enter into the calculation.…”
Section: A Deriving the Lindblad Equationmentioning
confidence: 99%
“…In general, simulations of single photon QWs in irregular arrays of waveguides are extremely difficult and therefore numerical solutions are necessary. Especially, if the propagation loss is included in numerically solving the Linblad equation it would require large resources including computing time and memory [40,41]. However, we can make use of the fact that single photon QWs do not exhibit any different behavior from classical wave propagation, and the light intensity distribution corresponds to the probability of detecting the photon at any position [42].…”
Section: Quantum Walks In Periodic and Quasiperiodic Multicore Ring Fmentioning
confidence: 99%
“…where H S is the system of interest Hamiltonian, H R is the reservoir Hamiltonian, and H SR is the system-reservoir interaction Hamiltonian. As shown in Refs [33][34][35]49], by tracing over the reservoir degrees of freedom, considering a bilinear interaction between system and reservoir, and under the Markov approximation, the system density operator ρ S has its evolution described by the Sudarshan-Lindblad master equation…”
Section: Evolution Equation For a N Spin-1/2 Particles Interactinmentioning
confidence: 99%
“…which satisfies the requirements T r 3 ρ 3 (1, 2, 3) = ρ 2 (1, 2), T r 2 ρ 3 (1, 2, 3) = ρ 2 (1, 3) and T r 1 ρ 3 (1, 2, 3) = ρ 2 (2, 3). By introducing the correlation operator (49) in Eq. (50) we get ρ 3 (1, 2, 3) ≈ ρ 1 (1)ρ 1 (2)ρ 1 (3) + ρ 1 (1)χ(2, 3) + ρ 1 (2)χ(1, 3) + ρ 1 (3)χ(1, 2).…”
Section: Beyond the Mean-field Approximationmentioning
confidence: 99%
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