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During the completion of this manuscript, an article of Creffield with related ideas has appeared. He shows how the quantum control of a periodic driving field can be employed to guide the motion of a boson in an otherwise empty optical lattice and to create entanglement by the interaction of two distinguishable bosons.
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During the completion of this manuscript, an article of Creffield with related ideas has appeared. He shows how the quantum control of a periodic driving field can be employed to guide the motion of a boson in an otherwise empty optical lattice and to create entanglement by the interaction of two distinguishable bosons.
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We will assume that the inhomogeneity Δ in Fig. 2 is zero, because otherwise the lattice has a net bias force and we cannot talk about a "ratchet".
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We will assume that the inhomogeneity Δ in Fig. 2 is zero, because otherwise the lattice has a net bias force and we cannot talk about a "ratchet".
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Note that we only specify the final time, but assume that the initial time is set at t=0.
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It is also possible to perform the optimization over a smaller subspace, using fewer vectors. This is particularly useful when one wants, for instance, to control the evolution of a single state.
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It is also possible to perform the optimization over a smaller subspace, using fewer vectors. This is particularly useful when one wants, for instance, to control the evolution of a single state.
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In the work of Ref. the ratchet is studied using the mean-field formalism for a Bose-Einstein condensate.
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In the work of Ref. the ratchet is studied using the mean-field formalism for a Bose-Einstein condensate.
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