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In the absence of external forcing, all trajectories on the phase plane of the van der Pol oscillator tend to a closed, periodic, trajectory -- the limit cycle -- after infinite time. Here, we drive the van der Pol oscillator with an external time-dependent force to reach the limit cycle in a given finite time. Specifically, we are interested in minimising the non-conservative contribution to the work when driving the system from a given initial point on the phase plane to any final point belonging to the limit cycle. There appears a speed limit inequality, which expresses a trade-off between the connection time and cost -- in terms of the non-conservative work. We show how the above results can be { generalized to the broader family of non-linear oscillators given by} the Liénard equation. Finally, we also look into the problem of minimising the total work done by the external force.
The dynamics of a system composed of elastic hard particles confined by an isotropic harmonic potential are studied. In the low-density limit, the Boltzmann equation provides an excellent description, and the system does not reach equilibrium except for highly specific initial conditions: it generically evolves toward and stays in a breathing mode. This state is periodic in time, with a Gaussian velocity distribution, an oscillating temperature, and a density profile that oscillates as well. We characterize this breather in terms of initial conditions and constants of the motion. For low but finite densities, the analysis requires taking into account the finite size of the particles. Under well-controlled approximations, a closed description is provided, which shows how equilibrium is reached at long times. The (weak) dissipation at work erodes the breather's amplitude, while concomitantly shifting its oscillation frequency. An excellent agreement is found between molecular dynamics simulation results and the theoretical predictions for the frequency shift. For the damping time, the agreement is not as accurate as for the frequency and the origin of the discrepancies is discussed.
The effective control of atomic coherence with cold atoms has made atom interferometry an essential tool for quantum sensors and precision measurements. The performance of these interferometers is closely related to the operation of large wave packet separations. We present here a novel approach for atomic beam splitters based on the stroboscopic stabilization of quantum states in an accelerated optical lattice. The corresponding Floquet state is generated by optimal control protocols. In this way, we demonstrate an unprecedented Large Momentum Transfer (LMT) interferometer, with a momentum separation of 600 photon recoils ($600\hbar k$) between its two arms. Each LMT beam splitter is realized in a remarkably short time (2 ms) and is highly robust against the initial velocity dispersion of the wave packet and lattice depth fluctuations. Our study shows that Floquet engineering is a promising tool for exploring new frontiers in quantum physics at large scales, with applications in quantum sensing and testing fundamental physics.
The monochromatic driving of a quantum system is a successful technique in quantum simulations, well captured by an effective Hamiltonian approach, and with applications in artificial gauge fields and topological engineering. Here, we investigate multichromatic Floquet driving for quantum simulation. Within a well-defined range of parameters, we show that the time coarse-grained dynamics of such a driven closed quantum system is encapsulated in an effective master equation for the time-averaged density matrix, that evolves under the action of an effective Hamiltonian and tunable Lindblad-type dissipation or quantum gain terms. As an application, we emulate the dissipation induced by phase noise and incoherent emission or absorption processes in the bichromatic driving of a two-level system, and reproduce the phase decoherence in a harmonic oscillator model.
Sujets
Engineering
Dynamical tunneling
Numerical methods
Field equations stochastic
Gaz quantique
Jet atomique
Effet tunnel assisté par le chaos
Quantum chaos
Puce atomique
Bose Einstein Condensation
Optical lattice
Optique atomique
Matter wave
Gaz quantiques
Mechanics
Optical tweezers
Effet rochet
Bragg Diffraction
Initial state
Bose-Einstein
Time dependence
Réseaux optiques
Plasmon polariton de surface
Dimension
Floquet theory
Couches mono-moléculaire auto assemblées
Optical lattices
Condensats de Bose Einstein
Quantum control
Collisions ultrafroides
Nano-lithographie
Non-adiabatic regime
Contrôle optimal quantique
Bose–Einstein condensates
Condensation de bose-Einstein
Constraint
Approximation semi-classique et variationnelle
Optical
Théorie de Floquet
Quantum
Cold atoms
Fluid
Bose-Einstein Condensate
Ouvertures métalliques sub-longueur d'onde
Chaos quantique
Mirror-magneto-optical trap
Contrôle optimal
Beam splitter
Fluorescence microscopy
Atom optics
Bragg scattering
Bose-Einstein condensates Coherent control Cold atoms and matter waves Cold gases in optical lattices
Current
Maxwell's demon
Hamiltonian
Periodic potentials
Condensat de Bose-Einstein
Mélasse optique
Levitodynamics
Atomic beam
Césium
Condensats de Bose– Einstein
Onde de matière
Matter waves
Réseau optique
Entropy production
Diffraction de Bragg
Lattice
Masques matériels nanométriques
Effet tunnel
Atomes ultrafroids dans un réseau optique
Espace des phases
Atom laser
Bose-Einstein condensate
Phase space
Fresnel lens
Microscopie de fluorescence
Ultracold atoms
Atom chip
Condensats de Bose-Einstein
Quantum collisions
Chaos
Condensat Bose-Einstein
Atomes froids
Bose-Einstein Condensates
Chaos-assisted tunneling
Piège magnéto-optique à miroir
Physique quantique
Optimal control theory
Effet tunnel dynamique
Experimental results
Bose Einstein condensate
Condensation
Optical molasses
Quantum optimal control
Lentille de Fresnel
Electromagnetic field
Nano-lithography
Bose-Einstein condensates