2010
DOI: 10.1140/epjb/e2010-00041-6
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Frequency-modulated ratchet with autoresonance

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Cited by 12 publications
(8 citation statements)
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“…With proper choice of the phase shift between the modulating signals, the driving force becomes a running plane wave experiencing time and space fluctuations. This kind of ratchets is known as travelling potential ratchets and considered in [40,41,42,43,44,45]. They can be used as quantum simulators of electron-phonon interactions in semiconducting materials [46,47,48,49].…”
Section: Introductionmentioning
confidence: 99%
“…With proper choice of the phase shift between the modulating signals, the driving force becomes a running plane wave experiencing time and space fluctuations. This kind of ratchets is known as travelling potential ratchets and considered in [40,41,42,43,44,45]. They can be used as quantum simulators of electron-phonon interactions in semiconducting materials [46,47,48,49].…”
Section: Introductionmentioning
confidence: 99%
“…Time-dependent perturbation V(x, t) leads to the nonintegrability of equations (16) and onset of chaos. For Γ = 0 and ε ≪ 1, chaotic motion occurs only inside a relatively small near-separatrix layer acting as a "bridge" between the domains of finite and ballistic motion.…”
Section: Classical Dynamicsmentioning
confidence: 99%
“…2. This asymmetry expects emergence of the nonzero ballistic flux [13,14,15,16] whose direction is determined by s. However, there is a large layer of regular motion in classical phase space, acting as a dynamical barrier for the atoms localized near the potential minima and preventing their transition into the ballistic regime. Consequently, atoms with minimal initial energies can produce directed current only due to tunneling which is almost negligible in deep optical lattices.…”
Section: Classical Dynamicsmentioning
confidence: 99%
“…On the classical level, such a perturbation can cause adiabatic transformation of the phase portrait, thereby driving atoms to the target state. A similar approach had been already used for producing Hamiltonian ratchets [12,13,14], as well as for cooling and partial localization of the particle ensemble in the vicinity of the minima of the potential [15]. In the present work we exploit almost the same idea for controlling quantum transport of atomic wavepackets in an optical lattice.…”
Section: Introductionmentioning
confidence: 99%