Research

Overview

In our lab we cool down atomic gases which are about a million times thinner than air to temperatures about a billionth of a degree above absolute zero. In these conditions quantum mechanical effects become essential: the atoms behave as matter waves which interfere, interact and can form very exotic states of matter such as superfluids, superconductors or quantum magnets. In some sense these phases are universal, as they appear in a broad range of other physical systems too, from liquid helium to complex solid-state materials, or even neutron stars.

Ultracold atomic gases provide an excellent platform to engineer the models underlying these phenomena, allowing us to study many-body quantum systems in a clean and very well controlled environment. On the one hand, they can be viewed as experimental quantum simulators for exploring challenging problems of condensed-matter physics such as neutron stars or high temperature superconductors. On the other hand, they also allow for the realization of completely novel systems of interesting properties, which do not exist in nature yet.

To learn more about our field of research you might want to read this Nature Physics review paper on quantum simulation in ultracold quantum gases.

Current research - Quantum liquid droplets in a mixture of Bose-Einstein condensates

Liquids are fluids of fixed volume and very low compressibility, which remain self-bound in the absence of external confinement. Their stability normally stems from the balance of attractive and repulsive forces deriving from different parts of the inter-particle interaction potential. The typical inter-particle distance is therefore fixed by the potential range, and corresponds to a dense phase. All liquids were thought to share this feature, independently of their classical or quantum nature. Recent experiments demonstrated however that a very different type of quantum liquid, more than eight orders of magnitude more dilute, could be created with ultracold magnetic atoms. In our group we have experimentally observed for the first time such a liquid using instead a weakly interacting mixture of Bose-Einstein condensates.

DropletsIn our experiments, we use two condensates of potassium that interact only through standard isotropic contact forces. We observe that the atoms form liquid self-bound droplets and directly measure their size and ultra-low density using high-resolution imaging. Moreover, we verify experimentally that the droplets are stabilized by repulsive forces stemming from quantum fluctuations. Finally, for small atom numbers we observe how quantum pressure dissociates the droplets into an expanding gas, and map out the liquid-to-gas transition.

The existence of this novel type of ultradilute quantum liquid is a direct manifestation of quantum effects in a weakly interacting system, and its properties do not depend on the microscopic details of the interactions between the atoms. Therefore, our droplets constitute an ideal platform for benchmarking complex quantum many-body theories beyond the mean-field approximation.
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Our droplet experiments have been performed in the quantum gas experiment that we have constructed at ICFO, starting in the winter 2014. As atomic species we use potassium, which has two bosonic isotopes and a fermionic one, allowing us to prepare degenerate quantum mixtures of bosonic or fermionic statistics. Furthermore, it offers an excellent control of the interatomic interactions thanks to favourable Feshbach resonances. Besides quantum liquid droplets, our setup should allow us to explore a broad range of physics problems, including for example polaron physics, topological physics and quantum magnetism in Fermi and spinor Bose gases.

Don’t hesitate to contact us if you want to learn more about our current and future research plans!

Ultracold fermions in optical lattices (in Tilman Esslinger’s lattice lab at ETH Zurich)

In experiments performed at ETH Zurich we studied the properties of a degenerate Fermi gas of potassium atoms loaded into an artificial crystal of light. This system behaves very similarly to the gas of electrons in a solid, the electrons being replaced by fermionic atoms, and the ion crystalline structure by an optical lattice made of interfering laser beams. It is indeed described by one of the key hamiltonians of condensed matter physics, the Fermi-Hubbard model, which contains extremely rich phenomena: metallic and insulating phases, magnetic order, superconductivity… Our system allows us to study the fascinating physics of strongly correlated materials (such as for example high-temperature superconductors) in a clean and highly controlled environment, where all relevant parameters – hopping, interaction strength, lattice geometry, filling – can be precisely adjusted. You will find a good review on Fermi-Hubbard physics with ultracold fermions in optical lattices here.

Sketch of a cloud of ultracold fermions in an optical lattice

One intriguing example of strongly correlated state that we have experimentally studied is the Mott insulator, which occurs for a system with a half-filled band. There, a strong repulsive interaction between two spin states can lead to a localization of the atoms in the lattice sites and drive the transition from a metallic to an insulating state (in the publications page you will find several links to our work on the topic). At low temperatures one expects the spin degrees of freedom to order as well forming an antiferromagnetic, Néel-like state.

artistic view of short range quantum magnetism with ultracold fermions in optical latticesRecently we have been able to observe for the first time the appearance of short-range magnetic correlations in such a system, and studied how they are favored by certain lattice geometries. This is an important step for simulating the physics of quantum magnets using ultracold atoms, and on the long term trying to address open questions in quantum magnetism using this approach.
For more information, you could have a look at our Science paper and this Science perspective. For a more general introduction, you might also find these links to Physics World and ETH Life useful.

Creating artificial solids using ultracold atoms also allows us to engineer completely new materials which do not exist in the solid state world.

merging Dirac points with ultracold fermions in honeycomb optical lattices

For example, by loading a non-interacting Fermi gas into a honeycomb structure, we realize artificial graphene and observe the presence of two Dirac points in the band structure. By tuning the geometry of the optical lattice we are able to adjust the properties of these Dirac points at will, moving them inside the Brillouin zone and changing the effective mass of the associated Dirac fermions. We can even observe how the two Dirac points annihilate each other when coming too close together, a situation which is presently out of reach in solid-state samples. By including interactions between the particles, these systems should also enable the study of “strongly correlated graphene” which otherwise does not exist in nature. For more information about these experiments you might want to read our Nature paper or this Nature News and Views. For general audience articles, check these Physics World and ETH Life links.

Superfluidity in ultracold Fermi gases (in Christophe Salomon’s lithium lab at ENS Paris)

In experiments performed at ENS Paris, we experimentally explored another classical problem of condensed matter physics: what is the fate of superconductivity in the presence of strong interactions between the particles?

artistic view of the BEC-BCS crossover in ultracold Fermi gasesSuperconductivity results from the superfluidity of the electron gas in a solid. Discovered in 1911 by Kammerlingh Onnes, it was only in 1957 that Bardeen, Cooper and Schrieffer managed to understand its microscopic origin. In a BCS superconductor, electrons form weakly bound pairs due to the effective attractive interactions mediated by their coupling to the lattice phonons. These Cooper pairs are stabilized by the presence of the Fermi sea and, as they are bosons, they can form a Bose-Einstein condensate which flows without resistance.

In the 80’s, Leggett, Nozières and Schmitt-Rink proposed a model unifying superfluidity in fermionic and bosonic systems. They showed that both phenomena could be understood as two limiting cases of the ground state of an attractive Fermi gas, the weakly interacting regime being associated to the BCS state and the strongly interacting limit corresponding to a Bose-Einstein condensate (BEC) of tightly bound dimers. In between, the BCS-BEC crossover is a regime of strong many-body quantum correlations that is extremely difficult to describe theoretically. Besides its fundamental interest, this regime is also believed to play a central role in some nuclear physics problems, describing for example the crust of neutron stars.

Ultracold Fermi gases have allowed for the realization of the BCS-BEC crossover, experimentally verifying the proposed scenario and making the quantitative study of this complex many-body problem possible. In the publications page you will find links to our early work on this topic. The experiments have nowadays reached such level of precision that they outperform classical computers and can be seen as true analog quantum computers (or quantum simulators) for this particular physics problem. You might want to have a look at the ENS Ultracold Fermi Gases Group to see the nice experiments they have recently done on the experimental setup that we built!