Transitionless quantum driving

By Michael V. Berry. 2009

920 citations recorded by the source corpus.

Subfields: Artificial Intelligence, Atomic and Molecular Physics, and Optics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/4593ceefb71a7a2b1f35b2f8449f4222e64fc038

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In Artificial Intelligence

In Atomic and Molecular Physics, and Optics

In Statistical and Nonlinear Physics

Citations in the corpus

Stimulated Raman adiabatic passage in physics, chemistry, and beyond (2016, background): “…in two- and three-state systems have been made by Demirplak and Rice (2003, 2005, 2008) with the name “assisted adiabatic passage by counterdiabatic field”, by Berry (2009) who used the term “transitionless quantum driving”, and by Chen et al. (2010) who named it “shortcut to adiabaticity”.”
High-fidelity quantum driving (2011, methodology): “[9] Berry, M.”
Reinforcement Learning in Different Phases of Quantum Control (2017, background): “[29] MV Berry, “Transitionless quantum driving,” Journal of Physics A: Mathematical and Theoretical 42, 365303 (2009).”
Shortcuts to Adiabaticity (2012, methodology): “Example 3: Population inversion in a two-level system (Berry, 2009; Chen et al., 2010c; Ibáñez et al., 2012a), see Sec.”
Shortcuts to adiabaticity: Concepts, methods, and applications (2019, methodology): “…2008) for internal state transfer using control fields, then rediscovered in a different but equivalent way as “Transitionless Tracking” by Berry (Berry, 2009), and used to design many control schemes after Chen et al. (2010a), unaware of the work of Demirplak and Rice, employed Berry’s method…”
Geometry and Response of Lindbladians (2015, background): “This path length is also applicable when one wants to simulate adiabatic evolution in a much shorter time (counterdiabatic or superadiabatic dynamics [197–199] or shortcuts to adiabaticity [200,201])”
Classical and Quantum Shortcuts to Adiabaticity for Scale-Invariant Driving (2014, methodology): “To this end, we use the formalism of generating functions, and unify previous approaches independently developed in classical and quantum studies.”
Accelerated quantum control using superadiabatic dynamics in a solid-state lambda system (2016, neutral): “ ΩÌ:P;A?Ü%Ä:ç;2Δ Ì Ê (4) the base adiabatic pulse for STIRAP is the ‘Vitanov’ shape23: 12 ΩÌ:P; = Ωcos kà:P; o ΩÉ:P; = Ωsin kà:P; o à:P; L è 2 1 1 ?:ç?Å:,/ (5) where Ω is the angular frequency of Rabi oscillations and the parameter å determines the rate of the adiabatic sweep. This shape is consider”