Our Research

Unlike traditional superconductivity in metals such as lead or aluminum, the unconventional superconductivity  in  the  heavy  fermions, cuprates, and  at  least  some  of  the  iron-based superconductors originates by doping a magnetic parent compound. This raises the possibility of carrier-doping-induced  quantum phase  transitions  in  these  systems arising  from  competing  types  of orders. As a result, the  extent  to which quantum  criticality  (QC) controls  the  finite  temperature properties  of  these  systems  have risen to the forefront in condensed matter physics, thus  triggering  a substantial  research  effort  devoted to  exploring  the  relationship between superconductivity  and magnetism  in  these systems.  While the pioneering work of 1958 by  Matthias  and  coworkers illustrates the antagonistic nature of these two phenomena, research efforts made to understand the unconventional superconductivity have revealed the coexistence of these competing orders in a certain space of the phase diagram of  unconventional  superconductors. The  study  of  the  interplay  between  magnetism  and superconductivity is crucial to understanding the nature of strongly correlated materials and this is, broadly,  the focus of research in our group. 

Heavy Fermions

Heavy-fermion (HF) materials have in recent years emerged as prototypical systems to study quantum  criticality, the  interaction  between  magnetism  and  superconductivity, and to address problems  that are central  to  the broader understanding of strongly correlated quantum matter. They offer a particularly propitious setting for these studies due to their unique properties. First, these materials contain both strongly localized (magnetic) and itinerant (conduction) electrons. Second,  strong  interactions  between  them  often  lead  to the competition  and  coexistence of different phases, such as antiferromagnetism, unconventional (non-Fermi liquid) metallic phase, and unconventional superconductivity. Thus a transition from localized to itinerant electron behavior happens across a quantum critical point (QCP) at T = 0 K (The picture to the left is from Aynajian et. al, Nature 486, 201–206, 2012) Third, their large effective  charge-carrier  mass  is accompanied by small relevant energy scales such that their ground state can be tuned not only by  chemical doping,  but  also  by  pressure  and  magnetic  fields  easily  accessible  in  a  typical condensed-matter  laboratory. 

Highlights of our research in this field are listed below: 

Strong Magnetic Fluctuations in a Superconducting State of CeCoIn5 

Non-Fermi liquid behavior with and without quantum criticality in Ce 1 − x Yb x CoIn 5

From local moment to mixed-valence regime in Ce(1-x)Yb(x)CoIn5 alloys

Iron based materials

The 2008 discovery of superconductivity in Fe-based pnictides, with the highest Tc reaching almost 60 K and, more recently, Fe chalcogenites were among the most significant breakthroughs in condensed-matter physics during the past decade. The reason is at least two fold: First, the phase diagram of Fe-based superconductors reveals an intricate interplay between magnetism and superconductivity, also typical of other “exotic” unconventional superconductors discovered in the last three decades of the last millennium: heavy fermions, cuprates, ruthenates, organic superconductors, and molecular superconductors. The research efforts made to understand the unconventional superconductivity in all these materials have revealed the coexistence of these competing orders in a certain space of their phase diagram. Second, this discovery of Fe-based high Tc superconductors has shown that the cuprates are not a unique class of materials (with the exception of the cuprates, the Tc of all the other unconventional superconductors is quite low) and that there is at least one other alternative to the CuO2 planes as the essential entity for the occurrence of high Tc superconductivity. Despite the tremendous progress made in understanding the physics of the cuprates, they have resisted, for more than 20 years, all attempts to formulate a comprehensive theory explaining all of their properties, in particular their high Tc. Now, with two species, Fe-pnictides/chalcogenites (FePn/Ch) and cuprates, to compare and contrast, the experiments could finally uncover the vital clues that theorists could use to solve the mystery of high transition temperature superconductivity. See schematic phase diagram from  Nature Physics 7, 272–276 (2011), showing similarities and differences between cuprates and pnictides

Highlight of our research in this field are listed below:

Filamentary superconductivity across the phase diagram of Ba(Fe,Co)2As2

Evidence for filamentary superconductivity nucleated at antiphase domain walls in antiferromagnetic CaFe2As2