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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.

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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.

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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.

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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.

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Sujets

Masques matériels nanométriques Optical lattice Fluid Contrôle optimal Non-adiabatic regime Onde de matière Nano-lithographie Bose-Einstein Quantum Ouvertures métalliques sub-longueur d'onde Optique atomique Engineering Approximation semi-classique et variationnelle Optical lattices Dynamical tunneling Mechanics Effet tunnel dynamique Hamiltonian Constraint Diffraction de Bragg Effet tunnel Effet rochet Fresnel lens Couches mono-moléculaire auto assemblées Condensation Quantum chaos Plasmon polariton de surface Condensat de Bose-Einstein Atomes ultrafroids dans un réseau optique Initial state Effet tunnel assisté par le chaos Condensat Bose-Einstein Entropy production Atomic beam Electromagnetic field Chaos-assisted tunneling Time dependence Condensats de Bose– Einstein Levitodynamics Quantum optimal control Optical molasses Condensats de Bose-Einstein Fluorescence microscopy Jet atomique Bose-Einstein condensates Césium Bose-Einstein Condensate Bragg scattering Experimental results Réseaux optiques Puce atomique Bose-Einstein Condensates Condensats de Bose Einstein Atom chip Espace des phases Physique quantique Lattice Phase space Atom optics Cold atoms Maxwell's demon Mélasse optique Réseau optique Nano-lithography Mirror-magneto-optical trap Matter wave Optimal control theory Lentille de Fresnel Field equations stochastic Chaos quantique Gaz quantique Quantum collisions Matter waves Current Piège magnéto-optique à miroir Quantum control Bose–Einstein condensates Optical tweezers Periodic potentials Chaos Optical Floquet theory Bose-Einstein condensates Coherent control Cold atoms and matter waves Cold gases in optical lattices Numerical methods Atom laser Bose Einstein condensate Atomes froids Microscopie de fluorescence Beam splitter Bose-Einstein condensate Condensation de bose-Einstein Théorie de Floquet Ultracold atoms Collisions ultrafroides Gaz quantiques Contrôle optimal quantique Dimension Bose Einstein Condensation Bragg Diffraction

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82