Christine Guerlin

Dicke quantum phase transition with a superfluid gas in an optical cavity

A phase transition describes the sudden change of state of a physical system, such as melting or freezing. Quantum gases provide the opportunity to establish a direct link between experiments and generic models that capture the underlying physics. The Dicke model describes a collective matter–light interaction and has been predicted to show an intriguing quantum phase transition. Here we realize the Dicke quantum phase transition in an open system formed by a Bose–Einstein condensate coupled to an optical cavity, and observe the emergence of a self-organized supersolid phase. The phase transition is driven by infinitely long-range interactions between the condensed atoms, induced by two-photon processes involving the cavity mode and a pump field. We show that the phase transition is described by the Dicke Hamiltonian, including counter-rotating coupling terms, and that the supersolid phase is associated with a spontaneously broken spatial symmetry. The boundary of the phase transition is mapped out in quantitative agreement with the Dicke model. Our results should facilitate studies of quantum gases with long-range interactions and provide access to novel quantum phases.

Dynamical coupling between a Bose–Einstein condensate and a cavity optical lattice

A Bose–Einstein condensate is dispersively coupled to a single mode of an ultra-high finesse optical cavity. The system is governed by strong interactions between the atomic motion and the light field even at the level of single quanta. While coherently pumping the cavity mode the condensate is subject to the cavity optical lattice potential whose depth depends nonlinearly on the atomic density distribution. We observe optical bistability already below the single photon level and strong back-action dynamics which tunes the coupled system periodically out of resonance.

Experimental investigation of transparent silicon carbide for atom chips

We investigate some properties of an atom chip made of a gold microcircuit deposited on a transparent silicon carbide substrate. A favorable thermal behavior is observed in the presence of electrical current, twice as good as a silicon counterpart. We obtain one hundred million rubidium atoms in a magneto-optical trap with several of the beams passing through the chip. We point out the importance of coating of the chip against reflection to avoid a temperature-dependent Fabry-Perot effect. We finally discuss detection through the chip, potentially granting large numerical apertures, as well as some other potential applications.

Symmetric microwave potentials for interferometry with thermal atoms on a chip

A trapped atom interferometer involving state-selective adiabatic potentials with two microwave frequencies on a chip is proposed. We show that this configuration provides a way to achieve a high degree of symmetry between the two arms of the interferometer, which is necessary for coherent splitting and recombination of thermal (i.e., noncondensed) atoms. The resulting interferometer holds promise to achieve high contrast and long coherence time, while avoiding the mean-field interaction issues of interferometers based on trapped Bose-Einstein condensates.

Splitting of trapped thermal atoms for atom-chip based interferometry

We present a design of an atom interferometer using thermal atoms trapped on a chip. We point-out that such an interferometer requires highly symmetrical potentials, and we propose a splitter based on microwave potentials with two coplanar waveguides to achieve this goal.

SYNTHETIC QUANTUM MANY-BODY SYSTEMS

This article discusses two different approaches to study the physics of quantum gases. We load a two-component Fermi gas of potassium atoms into an optical lattice and realize the Fermi-Hubbard model. We probe the crossover from a metal to a Mott insulator by measuring the number of doubly occupied lattice sites. A Bose-Einstein condensate placed into an ultrahigh-finesse optical cavity provides a many-body system with global interactions. We investigate this system in a regime where the physics of cavity optomechanics is revealed.