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Summary of Research Accomplishments

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<strong>Research</strong> Interests Qijin Chen Page 2 <strong>of</strong> 3<br />

Current <strong>Research</strong> Interests<br />

I have very broad research interests. For example, I have made significant scientific contributions<br />

in experimental condensed matter physics, and also had one year’s training in superstring theory.<br />

My primary focus is on the physics <strong>of</strong> superfluidity and related phenomena in ultracold atomic<br />

Fermi gases, while I am also interested in other areas outlined below.<br />

1. Ultracold atomic Fermi gases, optical lattices and quantum simulation<br />

Superfluidity in ultracold atomic Fermi gases is one <strong>of</strong> the most exciting research areas in condensed<br />

matter and atomic physics in recent years. Via Feshbach resonances, one can tune the<br />

attractive interaction between fermionic atoms from very weak to very strong. This makes it possible<br />

to observe Bose-Einstein condensation (BEC) in quantum degenerate Fermi gases directly<br />

over the entire range <strong>of</strong> the BCS-BEC crossover. Furthermore, this has created a strong hope that<br />

study <strong>of</strong> these systems may help us understand high Tc superconductivity. Another exciting tunable<br />

parameter in atomic Fermi gases is the population imbalance between the two spin species. The<br />

associated physics has turned out to be very rich. Added recently to this richness is the tunable<br />

mass ratio between the pairing atoms. Finally, optical lattices <strong>of</strong> atomic traps may be used to simulate<br />

typical as well as exotic condensed matter systems, e.g., the Hubbard model, so that study <strong>of</strong><br />

such simulated systems may provide a solution to unsolved problems in condensed matter physics.<br />

Even further, one can engineer many new systems to study exotic quantum phenomena.<br />

Over the past a few years, this field has seen very rapid progress. In 2003, the Jin group<br />

at JILA and the Grimm group at Universität Innsbruck, Austria made a big breakthrough and<br />

achieved molecular condensation in trapped atomic Fermi gases <strong>of</strong> 40 K and 6 Li, respectively. In<br />

2004, condensation <strong>of</strong> Cooper pairs was observed in 40 K by the Jin group and in 6 Li by the Grimm<br />

group and the Ketterle group at MIT. Evidence <strong>of</strong> superfluid phase transition were observed in<br />

thermodynamic behavior <strong>of</strong> 6 Li by the Thomas group at Duke and the Levin group in Chicago. In<br />

2005, the Ketterle group observed vortex lattices in 6 Li, which is the most definitive signature <strong>of</strong><br />

superfluidity. Population imbalance effects have become one <strong>of</strong> the hottest subjects since 2006, led<br />

by the MIT group and the Hulet group at Rice University. Since then, there has been a bloom in<br />

the study <strong>of</strong> optical lattices. Recently, synthetic gauge field and orbital effects in cold atoms have<br />

become new hot topics.<br />

A number <strong>of</strong> theorists have been working in the area <strong>of</strong> Fermi gases. However, their work has<br />

mostly been based on either the mean-field BCS-Leggett theory at zero temperature or the finite<br />

temperature Noziéres–Schmitt-Rink approach at Tc. The latter lacks self-consistency and cannot<br />

possibly predict a pseudogap. Other theoretical work has been based on the Bose liquid theory,<br />

and lacks proper treatment <strong>of</strong> the important fermionic pairing interaction.<br />

Our pairing fluctuation theory, originally developed for the pseudogap physics in high Tc superconductivity,<br />

has turned out very successful when applied to ultracold atomic Fermi gases. My<br />

current research includes fixing a couple <strong>of</strong> minor defects <strong>of</strong> this theory and apply it to more experiments<br />

or make more predictions. Of course, my research does not necessarily have to do with<br />

this theory. For example, one may proceed with completely different theories with optical lattices,<br />

synthetic gauge fields, etc.

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