2.5.2017  16:00, Raum: S288 
Dr. Igor I. Mazin
(U.S. Naval Research Laboratory, Washington D.C.)
Molecular orbitals vs. relativistic orbitals in t2g honeycomb lattices: SrRu2O6 as compared to Na2IrO3, RuCl3, and LiRuO3 

30.5.2017  16:00, Raum: S288 
Prof. Dr. Takahiro Onimaru
(Hiroshima University, Japan)
Exotic Quadrupolar Phenomena in NonKramers Doublets of Pr 1220 Systems 

20.6.2017  16:00, Raum: S288 
Dr. Kamran Behnia
(ESPCI, Paris)
Superconductivity and ferroelectricity in strontium titanate The largegap semiconductor strontium titanate (SrTiO3) becomes a metal upon removal of a tiny fraction of its oxygen atoms. The dilute metal has a sharp Fermi surface and is subject to a superconducting instability. Discovered halfacentury ago, the superconducting dome of strontium titanate remains doubly mysterious: How can superconductivity persist when there is only one carrier for 105 atoms and the Fermi energy an order of magnitude smaller then than the Debye energy? What destroys this cooperative order as soon as carrier density exceeds 0.02 electrons per formula unit? Our study of quantum oscillations as a function of carrier concentration documents the evolution of the Fermi surface as it evolves from singlepocket to multipocket and its correlation with structures in the superconducting dome. Our more recent study of superfluid density as a function of carrier concentration explores the second question. On the other hand, substituting strontium with calcium stabilizes a longrange ferroelectric order in Sr1xCaxTiO3. We find that in Sr1xCaxTiO_3delta ferroelectricity coexists with metallicity and its superconducting instability in a narrow window of doping. As the carrier concentration is increased, the ferroelectric order is eventually destroyed by a quantum phase transition. In the vicinity of this quantum phase transition, the superconducting critical temperature is enhanced. We will discuss its origin and a possible link to ferroelectric quantum criticality. 