Locally enhanced conductivity due to the tetragonal domain structure in LaAlO3/SrTiO3 heterointerfaces

  • Beena Kalisky
  • , Eric M. Spanton
  • , Hilary Noad
  • , John R. Kirtley
  • , Katja C. Nowack
  • , Christopher Bell
  • , Hiroki K. Sato
  • , Masayuki Hosoda
  • , Yanwu Xie
  • , Yasuyuki Hikita
  • , Carsten Woltmann
  • , Georg Pfanzelt
  • , Rainer Jany
  • , Christoph Richter
  • , Harold Y. Hwang
  • , Jochen Mannhart
  • , Kathryn A. Moler

Research output: Contribution to journalArticlepeer-review

185 Scopus citations

Abstract

The ability to control materials properties through interface engineering is demonstrated by the appearance of conductivity at the interface of certain insulators, most famously the {001} interface of the band insulators LaAlO 3 and TiO 2 -terminated SrTiO 3 (STO; refs,). Transport and other measurements in this system show a plethora of diverse physical phenomena. To better understand the interface conductivity, we used scanning superconducting quantum interference device microscopy to image the magnetic field locally generated by current in an interface. At low temperature, we found that the current flowed in conductive narrow paths oriented along the crystallographic axes, embedded in a less conductive background. The configuration of these paths changed on thermal cycling above the STO cubic-to-tetragonal structural transition temperature, implying that the local conductivity is strongly modified by the STO tetragonal domain structure. The interplay between substrate domains and the interface provides an additional mechanism for understanding and controlling the behaviour of heterostructures.

Original languageEnglish
Pages (from-to)1091-1095
Number of pages5
JournalNature Materials
Volume12
Issue number12
DOIs
StatePublished - Dec 2013

Bibliographical note

Funding Information:
We thank G. A. Sawatzky, N. Pavlenko, S. Ilani, Y. Yacoby and A. Vailionis for discussions, Y. Yeshurun and E. Zeldov for use of their optical set-ups, J. Drori, D. Hadad and Y. Shperber for their assistance with the optical measurements and M. E. Huber for assistance in SQUID design and fabrication. S. Ilani and collaborators have performed complementary measurements by local electrostatic imaging. This work was primarily supported by the Department of Energy, Office of Basic Energy Sciences, Materials Sciences and Engineering Division, under contract DE-AC02-76SF00515. B.K. acknowledges support from FENA and the EC grant no. FP7-PEOPLE-2012-CIG-333799. Y.W.X. acknowledges partial support from the US Air Force Office of Scientific Research (FAQSSO-10-1-0524). J.M. acknowledges financial support by the German Science Foundation (TRR80).

Funding

We thank G. A. Sawatzky, N. Pavlenko, S. Ilani, Y. Yacoby and A. Vailionis for discussions, Y. Yeshurun and E. Zeldov for use of their optical set-ups, J. Drori, D. Hadad and Y. Shperber for their assistance with the optical measurements and M. E. Huber for assistance in SQUID design and fabrication. S. Ilani and collaborators have performed complementary measurements by local electrostatic imaging. This work was primarily supported by the Department of Energy, Office of Basic Energy Sciences, Materials Sciences and Engineering Division, under contract DE-AC02-76SF00515. B.K. acknowledges support from FENA and the EC grant no. FP7-PEOPLE-2012-CIG-333799. Y.W.X. acknowledges partial support from the US Air Force Office of Scientific Research (FAQSSO-10-1-0524). J.M. acknowledges financial support by the German Science Foundation (TRR80).

FundersFunder number
FENA
German Science FoundationTRR80
Office of Basic Energy Sciences
National Science Foundation0957616
U.S. Department of Energy
Air Force Office of Scientific ResearchFAQSSO-10-1-0524
Seventh Framework Programme333799
Division of Materials Sciences and EngineeringDE-AC02-76SF00515
European Commission

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