Letter abstract


Nature Materials 7, 298 - 302 (2008)
Published online: 2 March 2008 | doi:10.1038/nmat2136

Subject Categories: Electronic materials | Nanoscale materials | Surface and thin films

Nanoscale control of an interfacial metal–insulator transition at room temperature

C. Cen1, S. Thiel2, G. Hammerl2, C. W. Schneider2, K. E. Andersen3, C. S. Hellberg3, J. Mannhart2 & J. Levy1

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Experimental1, 2, 3, 4, 5, 6, 7 and theoretical8, 9 investigations have demonstrated that a quasi-two-dimensional electron gas (q-2DEG) can form at the interface between two insulators: non-polar SrTiO3 and polar LaTiO3 (ref. 2), LaAlO3 (refs 3–5), KTaO3 (ref. 7) or LaVO3 (ref. 6). Electronically, the situation is analogous to the q-2DEGs formed in semiconductor heterostructures by modulation doping. LaAlO3/SrTiO3 heterostructures have recently been shown10 to exhibit a hysteretic electric-field-induced metal–insulator quantum phase transition for LaAlO3 thicknesses of 3 unit cells. Here, we report the creation and erasure of nanoscale conducting regions at the interface between two insulating oxides, LaAlO3 and SrTiO3. Using voltages applied by a conducting atomic force microscope (AFM) probe, the buried LaAlO3/SrTiO3 interface is locally and reversibly switched between insulating and conducting states. Persistent field effects are observed using the AFM probe as a gate. Patterning of conducting lines with widths of approx3 nm, as well as arrays of conducting islands with densities >1014 inch- 2, is demonstrated. The patterned structures are stable for >24 h at room temperature.

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  1. Department of Physics and Astronomy, University of Pittsburgh, 3941 O'Hara St., Pittsburgh, Pennsylvania 15260, USA
  2. Experimental Physics VI, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135, Augsburg, Germany
  3. Center for Computational Materials Science, Naval Research Laboratory, Washington, DC 20375, USA

Correspondence to: J. Levy1 e-mail: jlevy@pitt.edu




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