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Physical Review A

Time-reversal operation of tunneling dynamics of Bose-Einstein condensates in optical lattices

Noriaki Tsukada, Hiroyuki Yoshida, Takashi Suzuki

Published Jul 1, 2008• 3 citations
Publisher

Abstract

We propose schemes that can perform perfect time-reversal operation of the tunneling dynamics of Bose-Einstein condensates in optical lattices. One of the time-reversal schemes is to reverse the sign of the tunneling coefficient by a time-periodic potential, maintaining its magnitude at a constant value. The other scheme utilizes a staggered $0\text{\ensuremath{-}}\ensuremath{\pi}$ phase imprinting on the optical lattices. If the reversal of the tunneling coefficient or the phase imprinting is performed at $\ensuremath{\tau}={\ensuremath{\tau}}_{p}$, the initial distribution of the condensates is regained at $\ensuremath{\tau}=2{\ensuremath{\tau}}_{p}$. Although the nonlinear interatomic interaction deteriorates the fidelity of the time-reversal operation, if the sign of the nonlinearity is reversed simultaneously with the phase imprinting at $\ensuremath{\tau}={\ensuremath{\tau}}_{p}$, the time-reversal operation at $\ensuremath{\tau}=2{\ensuremath{\tau}}_{p}$ becomes nearly perfect.

DOI
10.1103/physreva.78.015601

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We propose schemes that can perform perfect time-reversal operation of the tunneling dynamics of Bose-Einstein condensates in optical lattices. One of the time-reversal schemes is to reverse the sign of the tunneling coefficient by a time-periodic potential, maintaining its magnitude at a constant value. The other scheme utilizes a staggered 0\ensuremath-\ensuremathπ0\text{\ensuremath{-}}\ensuremath{\pi}0\ensuremath-\ensuremathπ phase imprinting on the optical lattices. If the reversal of the tunneling coefficient or the phase imprinting is performed at \ensuremathτ=\ensuremathτp\ensuremath{\tau}={\ensuremath{\tau}}_{p}\ensuremathτ=\ensuremathτp​, the initial distribution of the condensates is regained at \ensuremathτ=2\ensuremathτp\ensuremath{\tau}=2{\ensuremath{\tau}}_{p}\ensuremathτ=2\ensuremathτp​. Although the nonlinear interatomic interaction deteriorates the fidelity of the time-reversal operation, if the sign of the nonlinearity is reversed simultaneously with the phase imprinting at \ensuremathτ=\ensuremathτp\ensuremath{\tau}={\ensuremath{\tau}}_{p}\ensuremathτ=\ensuremathτp​, the time-reversal operation at \ensuremathτ=2\ensuremathτp\ensuremath{\tau}=2{\ensuremath{\tau}}_{p}\ensuremathτ=2\ensuremathτp​ becomes nearly perfect.
Time reversal is an oft-used technique to probe and measure a quantum system. In particular, it is key for some theoretical information approaches to quantum criticality like fidelity decay. Here proposed is how to reverse the dynamics of cold bosonic atoms in an optical lattice in the regime described by the Bose-Hubbard model. The proposed experiment uses proven techniques—a linear phase imprint on the lattice, and a change in magnetic field to tune the boson-boson scattering length through a Feshbach resonance. The sensitivity of quantum dynamics across the insulator-superfluid quantum phase transition of the Bose-Hubbard model is studied, and sensing applications of dynamic reversals such as measuring the intensity of external potentials (e.g., gravity) is discussed.
The similarity between matter waves in periodic potential and solid-state physics processes has triggered the interest in quantum simulation using Bose-Fermi ultracold gases in optical lattices. The present work evidences the similarity between electrons moving under the application of oscillating electromagnetic fields and matter waves experiencing an optical lattice modulated by a frequency difference, equivalent to a spatially shaken periodic potential. We demonstrate that the tunneling properties of a Bose-Einstein condensate in shaken periodic potentials can be precisely controlled. We take additional crucial steps towards future applications of this method by proving that the strong shaking of the optical lattice preserves the coherence of the matter wavefunction and that the shaking parameters can be changed adiabatically, even in the presence of interactions. We induce reversibly the quantum phase transition to the Mott insulator in a driven periodic potential.