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Summary of Research Accomplishments

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<strong>Research</strong> Interests Qijin Chen Page 1 <strong>of</strong> 3<br />

RESEARCH INTERESTS<br />

<strong>Summary</strong> <strong>of</strong> <strong>Research</strong> <strong>Accomplishments</strong><br />

My research in the past several years has focused on superfluidity and superconductivity, beginning<br />

with high temperature superconductors and moving more recently to ultracold Fermi gases.<br />

In collaboration with my coworkers, I have previously developed a pairing fluctuation theory<br />

for the pseudogap physics in high Tc superconductors [Phys. Rev. Lett. 81, 4708 (1998), cited over<br />

130 times]. This theory naturally interpolates between the BCS and BEC limits, and extends the<br />

mean-field BCS theory to short coherence length superconductors in a natural way so that finitemomentum<br />

pairing fluctuations play a progressively more important role as the pairing strength<br />

increases. It has been successful in addressing many high Tc experiments, including, among others,<br />

the cuprate phase diagram and the highly unusual quasi-universal behavior <strong>of</strong> the superfluid<br />

density.<br />

Since 2005, I have extended our pairing fluctuation theory and applied it to trapped atomic<br />

Fermi gases. I have made great progress in this area. In collaboration with Holland et al. at JILA,<br />

we have performed the first theoretical study <strong>of</strong> pseudogap effects in atomic Fermi gases. We are<br />

the first that have introduced the concept <strong>of</strong> pseudogap into the field <strong>of</strong> atomic Fermi gases. We<br />

have successfully addressed the pairing gap in cold Fermi gas superfluids, the density pr<strong>of</strong>iles in<br />

a trap, the thermodynamic behavior in the strongly interacting regime, the phase diagrams with<br />

and without population imbalance, the collective mode behavior, etc. We have developed a theoretical<br />

thermometry based on adiabatic magnetic field sweeps. Importantly, the analysis <strong>of</strong> the<br />

specific heat measurements provides strong evidence for a superfluid phase transition. Recently,<br />

we have developed a theory for momentum resolved rf spectroscopy, our theory results are in good<br />

agreement with experiment. In particular, I propose that one can use the rf signal <strong>of</strong> minority<br />

fermions in the presence <strong>of</strong> phase separation at low T and high population imbalance to probe the<br />

homogeneous spectral function A(k, ω) <strong>of</strong> strongly interacting fermions.<br />

What is unique to my own research are a number <strong>of</strong> collaborations (and parallel papers) with<br />

leading experimentalists such as John Thomas at Duke University, Deborah Jin at JILA, Randall<br />

Hulet at Rice University, and Cheng Chin at Innsbruck and now the University <strong>of</strong> Chicago, as well<br />

as close interactions with the Ketterle group at MIT and Rudi Grimm group at Innsbruck, Austria.<br />

I have published more than 60 papers over my career. Since 2005, I have co-authored 4 review<br />

articles, written 1 Science paper, 7 Physical Review Letters, 11 Physical Review Rapid Communications,<br />

and 8 regular Physical Review A and B papers. Among them, the Science paper in<br />

collaboration with the Thomas group has been cited as one <strong>of</strong> several ground-breaking works in<br />

the field <strong>of</strong> ultracold Fermi gases. It has also been highlighted in Nature and discussed in Physics<br />

Today. Among other highlights is a collaboration with Debbie Jin which led to two publications.<br />

One <strong>of</strong> these [Phys. Rev. A 73, 041601(R) (2006)] was the first to show that her ground breaking<br />

experiments on the phase diagram are in good agreement with my theory.


<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.


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

2. Strongly correlated electrons<br />

I am interested in strongly correlated electron systems in general. The cuprates, organic, and<br />

heavy fermion (super)conductors are good examples <strong>of</strong> such systems. The new classes <strong>of</strong> Febased<br />

pnictide superconductors are believed to be strongly correlated as well. These systems call<br />

for new theories beyond the Landau Fermi liquid picture, which has been a foundation for modern<br />

solid state physics.<br />

High Tc, organic, heavy fermion and Fe-based pnictide superconductors<br />

High Tc superconductivity is arguably the greatest challenge in condensed matter physics. There<br />

has recently been a growing body <strong>of</strong> evidence which supports the relevance <strong>of</strong> precursor superconductivity,<br />

either through pairing fluctuations or vortex fluctuations, in the underdoped (pseudogapped)<br />

cuprates. Alternatively, new phases (e.g., antiferromagnet, insulating state) and quantum<br />

critical physics may come into play. There are more questions than answers. I am interested in<br />

any outstanding issues, such as the evolution <strong>of</strong> superfluid density with hole doping, transport<br />

properties, the superconductor-insulator transition at the lower critical doping, vortices and Nernst<br />

effects, Andreev reflection in the pseudogap regime, the one gap vs two gaps debate, etc.<br />

The phase diagrams <strong>of</strong> organic superconductors are very similar to those <strong>of</strong> the cuprates. There<br />

has been preliminary evidence for the existence <strong>of</strong> the pseudogap in these materials. The symmetry<br />

<strong>of</strong> the order parameter is still far from clear. Our theoretical explanation for the highly unusual T 3/2<br />

power law observed in the low T penetration depth measurements in the BEDT family has been an<br />

significant step toward understanding the symmetry and possible pseudogap phenomena in these<br />

superconductors. Heavy fermion superconductors also have similar phase diagrams, and some<br />

may exhibit quantum critical behavior. Interestingly, the discovery <strong>of</strong> Fe-based superconductors<br />

has invalidated the general belief that copper is the key to high Tc superconductivity whereas iron is<br />

<strong>of</strong>ten thought to be detrimental to superconductivity. It has now seemed to be a consensus that the<br />

order parameter <strong>of</strong> most Fe-based superconductors has an s± symmetry. Nevertheless, evidence<br />

for other symmetries to exist are also found in some materials. There are still many important<br />

questions to answer, including the most important pairing mechanism.<br />

3. Topological insulators, nanoscience, spintronics, and quantum computing<br />

Topological insulators have become a very hot field over the past couple <strong>of</strong> years. One important<br />

question is to find interesting physics beyond the single particle picture and find potential<br />

applications. Nanoscale physics, spintronics and quantum computing have great potentials for industrial<br />

applications. They are <strong>of</strong>ten interrelated. I have always been interested in these exciting<br />

areas. Optical lattices are also interrelated with nanoscale physics, quantum information science<br />

and quantum computing. One may use optical lattices to study topological insulators. In particular,<br />

the p + ip superfluid may be a topological superfluid, which can be used to study Majorana<br />

fermions. These Majorana fermions are believed to be able to be used for topological quantum<br />

computing.

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