Academic literature on the topic 'Non-Markovianity'

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Journal articles on the topic "Non-Markovianity"

1

Vacchini, Bassano, Andrea Smirne, Elsi-Mari Laine, Jyrki Piilo, and Heinz-Peter Breuer. "Markovianity and non-Markovianity in quantum and classical systems." New Journal of Physics 13, no. 9 (2011): 093004. http://dx.doi.org/10.1088/1367-2630/13/9/093004.

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2

Campbell, Steve, Maria Popovic, Dario Tamascelli, and Bassano Vacchini. "Precursors of non-Markovianity." New Journal of Physics 21, no. 5 (2019): 053036. http://dx.doi.org/10.1088/1367-2630/ab1ed6.

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3

Zhang, Jian-Song, and Ai-Xi Chen. "Non-Markovinity of single qubit channels: analytical and numerical methods." Canadian Journal of Physics 92, no. 3 (2014): 230–35. http://dx.doi.org/10.1139/cjp-2013-0276.

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We propose methods to calculate non-Markovianity of four typical single qubit channels including flip (bit-flip, phase-flip, and bit-phase flip channels), depolarizing, phase damping, and amplitude damping channels analytically. Explicit expressions of non-Markovianity for some single qubit channels are obtained. For general channels we propose the Euler parametrization representation of quantum states to calculate non-Markovianity numerically.
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4

Benatti, Fabio, and Luigi Brancati. "Quasi-Entropies and Non-Markovianity." Entropy 21, no. 10 (2019): 1020. http://dx.doi.org/10.3390/e21101020.

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We address an informational puzzle that appears with a non-Markovian open qubit dynamics: namely the fact that, while, according to the existing witnesses of information flows, a single qubit affected by that dissipative dynamics does not show information returning to it from its environment, instead two qubits do show such information when evolving independently under the same dynamics. We solve the puzzle by adding the so-called quasi-entropies to the possible witnesses of information flows.
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5

Luoma, Kimmo, and Jyrki Piilo. "Discrete dynamics and non-Markovianity." Journal of Physics B: Atomic, Molecular and Optical Physics 49, no. 12 (2016): 125501. http://dx.doi.org/10.1088/0953-4075/49/12/125501.

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6

Zhang, X. Y., X. L. Huang, and X. X. Yi. "Enhancement of non-Markovianity by interference of two reservoirs." International Journal of Quantum Information 13, no. 06 (2015): 1550048. http://dx.doi.org/10.1142/s0219749915500483.

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We study the effect of the interference between two independent non-Markovian reservoirs on the non-Markovianity of a two-level system. We find that the interference can enhance the non-Markovianity of the system. The additive master equation (ME) is invalid even if only one of the two reservoirs is non-Markovian, while it is a good approximation when all reservoirs are Markovian. We also derive the two states uniqueness for a two-level system coupled to structured reservoirs which maximize the measure of non-Markovianity defined by Breuer et al. [Phys. Rev. Lett. 103 (2009) 210401].
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7

Dijkstra, Arend G., and Yoshitaka Tanimura. "Non-Markovianity: initial correlations and nonlinear optical measurements." Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences 370, no. 1972 (2012): 3658–71. http://dx.doi.org/10.1098/rsta.2011.0203.

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By extending the response function approach developed in nonlinear optics, we analytically derive an expression for the non-Markovianity in the time evolution of a system in contact with a quantum mechanical bath, and find a close connection with the directly observable nonlinear optical response. The result indicates that memory in the bath-induced fluctuations rather than in the dissipation causes non-Markovianity. Initial correlations between states of the system and the bath are shown to be essential for a correct understanding of the non-Markovianity. These correlations are included in ou
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8

Yazaki, Tomoaki, Kiyoshi Kobayashi, and Akira Ishikawa. "Quantum non-Markovian dynamics controlled by a local nanoprobe in nanosystems coupled via optical near fields." Japanese Journal of Applied Physics 60, no. 12 (2021): 122008. http://dx.doi.org/10.35848/1347-4065/ac3523.

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Abstract The optical near field originates from the non-Markovianity of quantum coherent dynamics due to the light–matter interaction. To observe the optical near field localized near the surface of a nanomaterial, a local nanoprobe must be in close proximity, and the effect of the local nanoprobe cannot be ignored. Therefore, we elucidate the effect of the local nanoprobe on the non-Markovianity of the optical-near-field interaction, estimating the trace distance between the density matrices in the non-Markovian and Markovian cases and its integration as a quantitative measure of the non-Mark
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9

Kurt, Arzu. "Interplay between Non-Markovianity of Noise and Dynamics in Quantum Systems." Entropy 25, no. 3 (2023): 501. http://dx.doi.org/10.3390/e25030501.

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The non-Markovianity of open quantum system dynamics is often associated with the bidirectional interchange of information between the system and its environment, and it is thought to be a resource for various quantum information tasks. We have investigated the non-Markovianity of the dynamics of a two-state system driven by continuous time random walk-type noise, which can be Markovian or non-Markovian depending on its residence time distribution parameters. Exact analytical expressions for the distinguishability as well as the trace distance and entropy-based non-Markovianity measures are ob
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10

Milz, Simon, Felix A. Pollock, Thao P. Le, Giulio Chiribella, and Kavan Modi. "Entanglement, non-Markovianity, and causal non-separability." New Journal of Physics 20, no. 3 (2018): 033033. http://dx.doi.org/10.1088/1367-2630/aaafee.

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