Electronic reconstruction at an interface between a Mott insulator and a band insulator

Surface science is an important and well-established branch of materials science involving the study of changes in material properties near a surface or interface. A fundamental issue has been atomic reconstruction: how the surface lattice symmetry differs from the bulk. ‘Correlated-electron compounds’ are materials in which strong electron–electron and electron–lattice interactions produce new electronic phases, including interaction-induced (Mott) insulators, many forms of spin, charge and orbital ordering, and (presumably) high-transition-temperature superconductivity. Here we propose that the fundamental issue for the new field of correlated-electron surface/interface science is ‘electronic reconstruction’: how does the surface/interface electronic phase differ from that in the bulk? As a step towards a general understanding of such phenomena, we present a theoretical study of an interface between a strongly correlated Mott insulator and a band insulator. We find dramatic interface-induced electronic reconstructions: in wide parameter ranges, the near-interface region is metallic and ferromagnetic, whereas the bulk phase on either side is insulating and antiferromagnetic. Extending the analysis to a wider range of interfaces and surfaces is a fundamental scientific challenge and may lead to new applications for correlated electron materials.

[1]  L. Tjeng,et al.  Ultrathin oxide films on metals: new physics and new chemistry? , 2001 .

[2]  Ismail,et al.  Surface dynamics of the layered ruthenate Ca1.9Sr0.1RuO4 , 2004 .

[3]  Y. Tokura,et al.  Orbital physics in transition-metal oxides , 2000, Science.

[4]  H. Unoki,et al.  Dielectric Properties of SrTiO3at Low Temperatures , 1971 .

[5]  D. Sarma,et al.  Electronic structure of Ca1 − xSrxVO3: A tale of two energy scales , 2001, cond-mat/0105424.

[6]  Ismail,et al.  Ferromagnetism stabilized by lattice distortion at the surface of the p-wave superconductor Sr(2)RuO(4) , 2000, Science.

[7]  Terakura,et al.  Phase diagram of tetragonal manganites , 2000, Physical review letters.

[8]  Asano,et al.  Full-potential band calculations on YTiO3 with a distorted perovskite structure. , 1995, Physical review. B, Condensed matter.

[9]  Masatoshi Imada,et al.  Metal-insulator transitions , 1998 .

[10]  Fujimori,et al.  Unrestricted Hartree-Fock study of transition-metal oxides: Spin and orbital ordering in perovskite-type lattice. , 1995, Physical review. B, Condensed matter.

[11]  Akira Ohtomo,et al.  Artificial charge-modulationin atomic-scale perovskite titanate superlattices , 2002, Nature.

[12]  M. Potthoff,et al.  Metallic surface of a Mott insulator-Mott insulating surface of a metal , 1999 .

[13]  K. Müller,et al.  SrTi O 3 : An intrinsic quantum paraelectric below 4 K , 1979 .

[14]  H. Unoki,et al.  Dielectric Properties of SrTi O 3 at Low Temperatures , 1971 .

[15]  L. Tjeng,et al.  Photoemission evidence of electronic stabilization of polar surfaces in K3C60 , 2000 .

[16]  Okada,et al.  Optical spectra in (La,Y)TiO3: Variation of Mott-Hubbard gap features with change of electron correlation and band filling. , 1995, Physical review. B, Condensed matter.

[17]  L. Tjeng,et al.  Electronic structure and chemical reactivity of oxide-metal interfaces: MgO(100)/Ag(100) , 2000 .

[18]  A. Stoneham,et al.  CONDUCTIVITY AND NEGATIVE-U FOR IONIC GRAIN-BOUNDARIES , 1983 .

[19]  Y. Tokura,et al.  Perovskite superlattices as tailored materials of correlated electrons , 2001 .