A Surface-Tailored, Purely Electronic, Mott Metal-to-Insulator Transition

Author:

Moore R. G.1234,Zhang Jiandi1234,Nascimento V. B.1234,Jin R.1234,Guo Jiandong1234,Wang G.T.1234,Fang Z.1234,Mandrus D.1234,Plummer E. W.1234

Affiliation:

1. Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996, USA.

2. Department of Physics, Florida International University, Miami, FL 33199, USA.

3. Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA.

4. National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China.

Abstract

Mott transitions, which are metal-insulator transitions (MITs) driven by electron-electron interactions, are usually accompanied in bulk by structural phase transitions. In the layered perovskite Ca 1.9 Sr 0.1 RuO 4 , such a first-order Mott MIT occurs in the bulk at a temperature of 154 kelvin on cooling. In contrast, at the surface, an unusual inherent Mott MIT is observed at 130 kelvin, also on cooling but without a simultaneous lattice distortion. The broken translational symmetry at the surface causes a compressional stress that results in a 150% increase in the buckling of the Ca/Sr-O surface plane as compared to the bulk. The Ca/Sr ions are pulled toward the bulk, which stabilizes a phase more amenable to a Mott insulator ground state than does the bulk structure and also energetically prohibits the structural transition that accompanies the bulk MIT.

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference33 articles.

1. N. F. Mott, Proc. Phys. Soc. London Sect. A62, 416 (1949).

2. Metal Insulator Transitions 1974

3. Quantum Theory of Solids 1955

4. Metal-insulator transitions

5. Introduction to Condensed Matter Physics 2005

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