Strongly Correlated Electron Systems
Strongly correlated electron systems
Strongly correlated electron systems show some of the most intriguing and least understood phenomena of solid state physics, including high temperature superconductivity and quantum criticality. We develop new quantum field theoretical and computational methods for a better qualitative understanding and quantitative description of strongly correlated electron systems. Application-wise, our focus is on transition metal oxides and f-electron systems, both as bulk materials and heterostructures. Our research often tries to explain unusual experimental results, in other cases our insight as well as serendipity lead to the discovery of new physical phenomena or applications. In the following, four exemplary cases are highlighted.
A physical phenomena, we actually discovered by serendipity analyzing LDA+DMFT results for SrVO3 , are kinks in strongly correlated electron systems. Even absent any external bosonic degrees of freedom such as phonons or antiferromagnetic spin-fluctuations, there is a kink in the dispersion relation of strongly correlated materials. This could be explained mathematically  as necessitating from a three peak structure with a quasiparticle peak separated from the lower and upper Hubbard bands. More recently  we were able to pin-point the physical origin of the kink: the kink energy scale is nothing but the Kondo temperature, which for a lattice model such as the Hubbard model (transition metal oxides or f-electron systems) is different from the width of the quasiparticle peak.
Left: Usual Anderson impurity model with a single interacting site coupled via \(V\) to an uncorrelated and wide conduction electron band. In this case, the width of the central peak and the Kondo temperature are the same.
Right: Hubbard model situation, where an electron leaving a correlated site moves within the strongly correlated and narrow band. In this situation, the effective Kondo energy scale is smaller than the width of the narrow band. There is a kink at the Kondo energy scale.
 I. A. Nekrasov, K. Held, G. Keller, D. E. Kondakov, Th. Pruschke, M. Kollar, O. K. Andersen, V. I. Anisimov, and D. Vollhardt, Momentum-resolved spectral functions of SrVO3 calculated by LDA+DMFT, Phys. Rev. B 73, 155112 (2006)
 K. Byczuk, M. Kollar, K. Held, Y.-F. Yang, I. A. Nekrasov, Th. Pruschke, and D. Vollhardt, Kinks in the dispersion of strongly correlated electrons, Nature Physics 3, 168 (2007)
 K. Held, R. Peters, and A. Toschi, Poor Man’s Understanding of Kinks Originating from Strong Electronic Correlations, Phys. Rev. Lett. 110, 246402 (2013)
The isostructural metal-insulator transition in Cr-doped V2O3 is the textbook example of a Mott-Hubbard transition between a paramagnetic metal and a paramagnetic insulator. One of the first achievements of LDA+DMFT was the proper description of this Mott-Hubbard transition in V2O3 . Together with our experimental colleagues, we were recently able to shed new light [5,6] on this famous transition. In particular, the old paradigm of a doping-pressure equivalence does not hold, and there is a microscale phase separation for Cr-doped V2O3.
The metallic phase of Cr-doped V2O3 is actually a mixture of metallic (red) and insulating (blue) islands, phase-separated on the microscale .
 K. Held, G. Keller, V. Eyert, D. Vollhardt, and V.I. Anisimov, Mott-Hubbard Metal-Insulator Transition in Paramagnetic V2O3: a LDA+DMFT(QMC) Study, Phys. Rev. Lett. 86, 5345 (2001)
 P. Hansmann, A. Toschi, G. Sangiovanni, T. Saha-Dasgupta, S. Lupi, M. Marsi, K. Held, Mott-Hubbard transition in V2O3 revisited, Phys. Status Solidi B 250, No. 7, 1251–1264 (2013)
 S. Lupi, L. Baldassarre, B. Mansart, A. Perucchi, A. Barinov, P. Dudin, E. Papalazarou, F. Rodolakis, J. -P. Rueff, J. -P. Itié, S. Ravy, D. Nicoletti, P. Postorino, P. Hansmann, N. Parragh, A. Toschi, T. Saha-Dasgupta, O. K. Andersen, G. Sangiovanni, K. Held, and M. Marsi, A microscopic view on the Mott transition in chromium-doped V2O3, Nature Communications 1, 105 (2010)
A fascinating source of green energy is the transformation of heat (gradients) into electric energy through the Seebeck effect. Our quest in this research field is the design of new materials with a higher thermoelectric figure of merit. This is needed for a higher efficiency and wide scale technological application. We are studying various materials such as FeSb2 and NaxCoO2, with the aim of understanding the microscopic origin of why the thermopower in some materials is particularly high and how one can further optimize it.
Figure 3: If we apply a heat gradient, electrons and holes alike are diffusing from the hot to the cold side resulting typically in a very small net current. For a good thermoelectric, we need however a large net current, i.e. a huge asymmetry between electron and hole diffusion. Due to the pudding-mold bandstructure in NaxCoO2, the group velocity of the holes is already considerably larger than that of the electrons, as indicated by the larger orange arrow. Electronic correlations additionally shift electrons away from the Fermi level, as visualized by the fewer blue electrons and the narrower width of the blue arrow. As both effects add up, the electron current is much smaller than the hole current leading to the net current displayed, and hence to the good thermoelectric properties of NaxCoO2 .
 P. Wissgott, A.Toschi, H. Usui, K. Kuroki, and K. Held, Enhancement of the NaxCoO2 thermopower due to electronic correlations, Phys. Rev. B 82, 201106(R) (2010)
With the wizardry of modern molecular beam epitaxy and pulsed laser deposition growing oxide heterostructures atomic-layer by atomic-layer, a new field of solid state research emerged. Many oxide heterostructures, including the LaAlO3/SrTiO3 prototype, have only lightly doped d-bands, and are hence not strongly correlated. In such a case, a density functional theory description and even a tight-binding modelling  is sufficient. We have developed a theory for spin-orbit coupling in oxide heterostructures, which allows us to explain why the spin splitting can be particularly strong and angle dependent in oxide heterostructures . In other cases, the number of d-electrons on the Vanadium sites is substantial, and electronic correlations are strong. For example, a few SrVO3 layers on a substrate such as SrTiO3 are Mott insulating whereas bulk SrVO3 is a (strongly correlated) metal. This can be even used to build a Mott transistor, where an electric field triggers a metal-insulator transition . The alternating atomic layers of oxide heterostructures often lead to a polar surface and we have proposed to exploit this polar surface along with the conducting interface layer and the large optical absorption in LaAlO3|SrTiO3heterostructures, for solar cell applications. Subsequent experiments on different heterostructures showed a large photovoltage and hence confirm the proposed mechanism.
Figure 4: Schematic of an oxide heterostructure solar cell. Phonons are absorbed in the LaMO3 absorber material. The polar electric field separates the created electrons and holes: the electrons are accelerated to the conducting interface and the holes to the surface. Exploiting the flexibility of oxide heterostructures to grow materials with different gaps, here LaMO3 and LaM’O3, allows for further boosting the solar cell’s efficiency .
 Z. Zhong, Q. Zhang, and K. Held, Quantum confinement in perovskite oxide heterostructures: tight binding instead of nearly free electron picture, Phys. Rev. B 88, 125401 (2013)
 Z. Zhong, A. Toth, and K. Held, Theory of spin-orbit coupling at LaAlO3/SrTiO3 interfaces and SrTiO3 surfaces, Phys. Rev. B 87, 161102 (2013)
 Z. Zhong, M. Wallerberger, J. M. Tomczak, C. Taranto, N. Parragh, A. Toschi, G. Sangiovanni, and K. Held, Electronics with correlated oxides: SrVO3/SrTiO3 as a Mott transistor, arXiv:1312.5989
 E. Assmann, P. Blaha, R. Laskowski, K. Held, S. Okamoto, and G. Sangiovanni, Oxide Heterostructures for Efficient Solar Cells, Phys. Rev. Lett. 110, 078701 (2013)