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arXiv:1802.05476 · Journal of Physics A Mathematical and Theoretical

Quantum walks of kicked Bose–Einstein condensates

Caspar Groiseau, Alexander Gresch, Sandro Wimberger

Published May 17, 2018• 10 citations
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Abstract

Abstract We analytically investigate the recently proposed and implemented discrete-time quantum walk based on kicked ultra-cold atoms. We show how the internal level structure of the kicked atoms leads to the emergence of a relative light-shift phase immediately relevant for the experimental realization. Analytical solutions are provided for the momentum distribution for both the case of quantum resonance and the near-resonant quasimomenta.

DOI
10.1088/1751-8121/aac5d5

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Abstract We analytically investigate the recently proposed and implemented discrete-time quantum walk based on kicked ultra-cold atoms. We show how the internal level structure of the kicked atoms leads to the emergence of a relative light-shift phase immediately relevant for the experimental realization. Analytical solutions are provided for the momentum distribution for both the case of quantum resonance and the near-resonant quasimomenta.
Randomness is the essence of many processes in nature and human society. It can provide important insights into phenomena as diverse as disease transmission, financial markets, and signal processing. Quantum randomness is intrinsically different from classical stochasticity since it is affected by interference and entanglement. Quantum walks profit from the entanglement that is built up between a walker's position and the "coin" degree of freedom that determines the direction of a walker's motion. This entanglement makes quantum walks promising candidates for the implementation of quantum computational algorithms and as a detector of quantum behavior. While several proof-of-principle quantum walk experiments have recently been implemented, the walk scheme we demonstrate here involves the synthesis of the atom-optics kicked rotor with the dynamics of a state selective ratchet realized with a Bose-Einstein condensate. Here we present a discrete-time quantum walk that uses the momentum of ultra-cold rubidium-87 atoms as the walk space and two internal atomic states as the coin degree of freedom. To implement each step of the walk, i.e. a coin toss followed by a unitary shift operator, we use a microwave pulse, which produces a superposition of two internal states, and a resonant quantum ratchet, which entangles the internal and external degrees of freedom. Our quantum ratchet, whose direction at each step depends on the result of the coin toss, is realized by the atom-optics kicked rotor. We demonstrate the principle features of a standard quantum walk, contrasting them to the behavior of a classical walk. In addition, by manipulating either the walk or coin operator we show how the walk dynamics can be biased or reversed. Furthermore, we show the quantum-to-classical transition in our walk, via randomizing the mixing between the two internal states during each coin toss. Our walk offers distinct advantages arising from the robustness of its dynamics in momentum space, extendability to higher dimensions, and possible dependence on many-body correlations.
Over the last decade there have been many advances in studies of quantum walks (QWs) including a momentum-space QW recently realized in our spinor Bose-Einstein condensate system. This QW possessed behaviors that generally agreed with theoretical predictions; however, it also showed momentum distributions that were not adequately explained by the theory. We present a theoretical model which proves that the coherent dynamics of the spinor condensate is sufficient to explain the experimental data without invoking the presence of a thermal cloud of atoms as in the original theory. Our numerical findings are supported by an analytical prediction for the momentum distributions in the limit of zero-temperature condensates. This current model provides more complete explanations to the momentum-space QWs that can be applied to study quantum search algorithms and topological phases in Floquet-driven systems.
The kicking sequence of the atom-optics kicked rotor at quantum resonance can be interpreted as a quantum random walk in momentum space. We show how such a walk can become the basis for nontrivial classical walks by applying a random sequence of intensities and phases of the kicking lattice chosen according to a probability distribution. This distribution converts on average into the final momentum distribution of the kicked atoms. In particular, it is shown that a power-law distribution for the kicking strengths results in a L\'evy walk in momentum space and in a power law with the same exponent in the averaged momentum distribution. Furthermore, we investigate the stability of our predictions in the context of a realistic experiment with Bose-Einstein condensates.
We have observed high-order quantum resonances in a realization of the quantum delta-kicked rotor, using Bose-condensed Na atoms subjected to a pulsed standing wave of laser light. These resonances occur for pulse intervals that are rational fractions of the Talbot time, and are characterized by ballistic momentum transfer to the atoms. The condensate's narrow momentum distribution not only permits the observation of the quantum resonances at 3/4 and 1/3 of the Talbot time, but also allows us to study scaling laws for the resonance width in quasimomentum and pulse interval.
We experimentally explore the underlying pseudoclassical phase space structure of the quantum delta-kicked accelerator. This was achieved by exposing a Bose-Einstein condensate to the spatially corrugated potential created by pulses of an off-resonant standing light wave. For the first time quantum accelerator modes were realized in such a system. By utilizing the narrow momentum distribution of the condensate we were able to observe the discrete momentum state structure of a quantum accelerator mode and also to directly measure the size of the structures in the phase space.