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Quantum ratchets for quantum communication with optical superlattices

Oriol Romero-Isart and Juan José García-Ripoll
Phys. Rev. A 76, 052304 – Published 6 November 2007

Abstract

We propose to use a quantum ratchet to transport quantum information in a chain of atoms trapped in an optical superlattice. The quantum ratchet is created by a continuous modulation of the optical superlattice which is periodic in time and in space. Though there is zero average force acting on the atoms, we show that indeed the ratchet effect permits atoms on even and odd sites to move along opposite directions. By loading the optical lattice with two-level bosonic atoms, this scheme permits us to perfectly transport a qubit or entangled state imprinted in one or more atoms to any desired position in the lattice. From the quantum computation point of view, the transport is achieved by a smooth concatenation of perfect swap gates. We analyze setups with noninteracting and interacting particles and in the latter case we use the tools of optimal control to design optimal modulations. We also discuss the feasibility of this method in current experiments.

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  • Received 3 October 2007
  • Publisher error corrected 12 November 2007

DOI:https://doi.org/10.1103/PhysRevA.76.052304

©2007 American Physical Society

Corrections

12 November 2007

Erratum

Authors & Affiliations

Oriol Romero-Isart

  • Departament de Física, Grup de Física Teòrica, Universitat Autònoma de Barcelona, E-08193 Bellaterra, Spain

Juan José García-Ripoll

  • Facultad de CC. Físicas, Universidad Complutense de Madrid, Ciudad Universitaria s/n, Madrid E-28040, Spain

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Issue

Vol. 76, Iss. 5 — November 2007

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Images

  • Figure 1
    Figure 1
    (Color online) An optical superlattice arises from a combination of two potentials with different periods. By modulating the depths and displacements of these potentials we can raise and lower the tunneling rates between odd and even pairs of sites (red arrows). This way, by means of perfect swaps, the state of a particle can be transported along the lattice.Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) (a) Model case of two lattice sites disconnected from the rest because J2=0. By fixing the hopping between wells to a precise value J for a time T, it is possible to swap the atoms. Note that the doubly occupied sites have more energy due to the interaction U and a possible inhomogeneity of the lattice potential Δ. (b) Combining the solution for a pair of sites we obtain one possible modulation of the hoppings J1 (solid) and J2 (dashed), namely, J1 and J2 are square waves in antiphase. This produces the quantum transport. (c) Values of J and T for which perfect transport is achieved. Each circle is a solution; the solid line joins the solutions with smallest hopping and the dashed line is the solution for noninteracting particles.Reuse & Permissions
  • Figure 3
    Figure 3
    (Color online) (a) Hopping and (b) fidelity of the gate (F=|01|U(t)|10|2) with the perfect transport for half a period [0,T) during which J1(t)=J(t) and J2=0. We find two solutions, one for T=2πU (solid) and another one for T=4πU (dashed), with three and two modes, respectively. In (c) we plot the corresponding modulations of the superlattice.Reuse & Permissions
  • Figure 4
    Figure 4
    (Color online) On the upper figure we plot a solution of J1(t) (solid) and J2(t) (dashed) for a perfect transport of the qubit. In the lower figure we plot the average position of the qubit on the lattice as transported by these modulations. These plots have been computed using T=4πU.Reuse & Permissions
  • Figure 5
    Figure 5
    (Color online) Parameters of the double well potential as a function of the superlattice modulation ΔV=(Vx+V2)2. We plot the effective hopping between wells J (dash-dot, right axis), the energy gap to higher bands ΔE (dashed), and the on-site interaction u (solid). Everything is expressed in units of the recoil energy Er.Reuse & Permissions
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