Loading...
Derniers dépôts, tout type de documents
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.
We numerically study the optimal control of an atomic Bose-Einstein condensate in an optical lattice. We present two generalizations of the gradient-based algorithm, GRAPE, in the non-linear case and for a two-dimensional lattice. We show how to construct such algorithms from Pontryagin’s maximum principle. A wide variety of target states can be achieved with high precision by varying only the laser phases setting the lattice position. We discuss the physical relevance of the different results and the future directions of this work.
Microscopically probing quantum many-body systems by resolving their constituent particles is essential for understanding quantum matter. In most physical systems, distinguishing individual particles, such as electrons in solids, or neutrons and quarks in neutron stars, is impossible. Atombased quantum simulators offer a unique platform that enables the imaging of each particle in a many-body system. Until now, however, this capability has been limited to quantum systems in discretized space such as optical lattices and tweezers, where spatial degrees of freedom are quantized. Here, we introduce a novel method for imaging atomic quantum many-body systems in the continuum, allowing for in situ resolution of every particle. We demonstrate the capabilities of our approach on a two-dimensional atomic Fermi gas. We probe the density correlation functions, resolving their full spatial functional form, and reveal the shape of the Fermi hole arising from Pauli exclusion as a function of temperature. Our method opens the door to probing strongly-correlated quantum gases in the continuum with unprecedented spatial resolution, providing in situ access to spatially resolved correlation functions of arbitrarily high order across the entire system.
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.
Sujets
Diffraction de Bragg
Microscopie de fluorescence
Bose-Einstein Condensates
Piège magnéto-optique à miroir
Atom optics
Plasmon polariton de surface
Chaos
Réseau optique
Levitodynamics
Effet rochet
Quantum chaos
Approximation semi-classique et variationnelle
Bose-Einstein Condensate
Effet tunnel assisté par le chaos
Chaos-assisted tunneling
Entropy production
Beam splitter
Mélasse optique
Atomic beam
Gaz quantique
Dimension
Nano-lithography
Optical molasses
Effet tunnel dynamique
Physique quantique
Bose Einstein Condensation
Contrôle optimal quantique
Electromagnetic field
Condensats de Bose-Einstein
Optimal control theory
Fluid
Bose-Einstein condensates
Lattice
Couches mono-moléculaire auto assemblées
Césium
Maxwell's demon
Ultracold atoms
Constraint
Puce atomique
Optical lattices
Condensats de Bose– Einstein
Dynamical tunneling
Collisions ultrafroides
Espace des phases
Time dependence
Ouvertures métalliques sub-longueur d'onde
Bragg scattering
Phase space
Bragg Diffraction
Field equations stochastic
Contrôle optimal
Jet atomique
Periodic potentials
Théorie de Floquet
Current
Optical
Initial state
Bose-Einstein
Fresnel lens
Floquet theory
Bose Einstein condensate
Masques matériels nanométriques
Bose-Einstein condensate
Condensats de Bose Einstein
Condensat Bose-Einstein
Matter waves
Experimental results
Optical tweezers
Bose–Einstein condensates
Onde de matière
Engineering
Condensat de Bose-Einstein
Gaz quantiques
Effet tunnel
Atom laser
Matter wave
Lentille de Fresnel
Cold atoms
Non-adiabatic regime
Bose-Einstein condensates Coherent control Cold atoms and matter waves Cold gases in optical lattices
Chaos quantique
Mechanics
Atomes ultrafroids dans un réseau optique
Mirror-magneto-optical trap
Quantum
Atomes froids
Optique atomique
Optical lattice
Atom chip
Fluorescence microscopy
Nano-lithographie
Quantum optimal control
Condensation
Quantum collisions
Numerical methods
Condensation de bose-Einstein
Quantum control
Réseaux optiques
Hamiltonian