Author
Listed:
- T.C. Asmara
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
Singapore Synchrotron Light Source, National University of Singapore)
- A. Annadi
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore)
- I. Santoso
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
Singapore Synchrotron Light Source, National University of Singapore)
- P.K. Gogoi
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
Singapore Synchrotron Light Source, National University of Singapore)
- A. Kotlov
(Hamburger Synchrotronstrahlungslabor (HASYLAB) at Deutsches Elektronen-Synchrotron (DESY))
- H.M. Omer
(Singapore Synchrotron Light Source, National University of Singapore)
- M. Motapothula
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
Center for Ion Beam Applications (CIBA), National University of Singapore)
- M.B.H. Breese
(National University of Singapore
Singapore Synchrotron Light Source, National University of Singapore
Center for Ion Beam Applications (CIBA), National University of Singapore)
- M. Rübhausen
(NUSNNI-NanoCore, National University of Singapore
Institut für Angewandte Physik, Universität Hamburg
Center for Free Electron Laser Science (CFEL))
- T. Venkatesan
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
National University of Singapore)
- Ariando
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore)
- A. Rusydi
(NUSNNI-NanoCore, National University of Singapore
National University of Singapore
Singapore Synchrotron Light Source, National University of Singapore)
Abstract
In condensed matter physics the quasi two-dimensional electron gas at the interface of two different insulators, polar LaAlO3 on nonpolar SrTiO3 (LaAlO3/SrTiO3) is a spectacular and surprising observation. This phenomenon is LaAlO3 film thickness dependent and may be explained by the polarization catastrophe model, in which a charge transfer of 0.5e− from the LaAlO3 film into the LaAlO3/SrTiO3 interface is expected. Here we show that in conducting samples (≥4 unit cells of LaAlO3) there is indeed a ~0.5e− transfer from LaAlO3 into the LaAlO3/SrTiO3 interface by studying the optical conductivity in a broad energy range (0.5–35 eV). Surprisingly, in insulating samples (≤3 unit cells of LaAlO3) a redistribution of charges within the polar LaAlO3 sublayers (from AlO2 to LaO) as large as ~0.5e− is observed, with no charge transfer into the interface. Hence, our results reveal the different mechanisms for the polarization catastrophe compensation in insulating and conducting LaAlO3/SrTiO3 interfaces.
Suggested Citation
T.C. Asmara & A. Annadi & I. Santoso & P.K. Gogoi & A. Kotlov & H.M. Omer & M. Motapothula & M.B.H. Breese & M. Rübhausen & T. Venkatesan & Ariando & A. Rusydi, 2014.
"Mechanisms of charge transfer and redistribution in LaAlO3/SrTiO3 revealed by high-energy optical conductivity,"
Nature Communications, Nature, vol. 5(1), pages 1-10, May.
Handle:
RePEc:nat:natcom:v:5:y:2014:i:1:d:10.1038_ncomms4663
DOI: 10.1038/ncomms4663
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