2013
DOI: 10.1103/physrevlett.110.190601
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Electric Quantum Walks with Individual Atoms

Abstract: We report on the experimental realization of electric quantum walks, which mimic the effect of an electric field on a charged particle in a lattice. Starting from a textbook implementation of discrete-time quantum walks, we introduce an extra operation in each step to implement the effect of the field. The recorded dynamics of such a quantum particle exhibits features closely related to Bloch oscillations and interband tunneling. In particular, we explore the regime of strong fields, demonstrating contrasting … Show more

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Cited by 182 publications
(218 citation statements)
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“…This makes them valuable in quantum search algorithms [2] or even for general quantum computing [3]. Experiments on quantum walks range from realizations on trapped ions [4][5][6], to cold atoms in optical lattices [7][8][9], to light on an optical table [10][11][12][13][14][15], but there have been many other experimental proposals [16,17].…”
Section: Introductionmentioning
confidence: 99%
“…This makes them valuable in quantum search algorithms [2] or even for general quantum computing [3]. Experiments on quantum walks range from realizations on trapped ions [4][5][6], to cold atoms in optical lattices [7][8][9], to light on an optical table [10][11][12][13][14][15], but there have been many other experimental proposals [16,17].…”
Section: Introductionmentioning
confidence: 99%
“…Discrete-time quantum walks (DTQW) 6 , quantum mechanical generalizations of random walks, have in the recent years enjoyed increasing attention from both theoretical and experimental [7][8][9][10][11][12][13] physicists. The hallmark property of DTQWs is that they spread faster than classical random walks: on a regular graph, the variance of the position of the walker scales as O(t 2 ) with the number t of timesteps, rather than O(t) as in the classical case.…”
Section: Introductionmentioning
confidence: 99%
“…For example, Felix Bloch predicted in his seminal paper 5 that a crystal electron carries out an oscillatory motion under the influence of an external static electric field. While scattering of the electron prevents Bloch oscillations in bulk crystals, they have been observed in a number of equivalent systems, such as semiconductor superlattices 6 , atomic systems 7,8 , arrays of coupled dielectric waveguides 9,10 and periodic dielectric systems 11 . Other examples for the ability to map wave phenomena among different physical systems are Zener tunnelling in optical lattices 12,13 , as well as the analogy between the ballistic motion of an electronic wave packet in a tight-binding lattice 14 and discrete diffraction of light in a waveguide array 15,16 .…”
mentioning
confidence: 99%