Display options
Cite
Maniv E, Shalom MB, Ron A, et al. Strong correlations elucidate the electronic structure and phase diagram of LaAlO3/SrTiO3 interface. Nat Commun. 2015;6:8239doi: 10.1038/ncomms9239.
Maniv, E., Shalom, M. B., Ron, A., Mograbi, M., Palevski, A., Goldstein, M., & Dagan, Y. (2015). Strong correlations elucidate the electronic structure and phase diagram of LaAlO3/SrTiO3 interface. Nature communications, 68239. https://doi.org/10.1038/ncomms9239
Maniv, E, et al. "Strong correlations elucidate the electronic structure and phase diagram of LaAlO3/SrTiO3 interface." Nature communications vol. 6 (2015): 8239. doi: https://doi.org/10.1038/ncomms9239
Maniv E, Shalom MB, Ron A, Mograbi M, Palevski A, Goldstein M, Dagan Y. Strong correlations elucidate the electronic structure and phase diagram of LaAlO3/SrTiO3 interface. Nat Commun. 2015 Sep 11;6:8239. doi: 10.1038/ncomms9239. PMID: 26359206; PMCID: PMC4647855.
Copy Download .nbib Format: NLM
Share it on

Nat Commun. 2015 Sep 11;6:8239. doi: 10.1038/ncomms9239.

Strong correlations elucidate the electronic structure and phase diagram of LaAlO3/SrTiO3 interface.

Nature communications

E Maniv, M Ben Shalom, A Ron, M Mograbi, A Palevski, M Goldstein, Y Dagan

Affiliations

  1. Raymond and Beverly Sackler School of Physics and Astronomy, Tel-Aviv University, Levanon Street, Tel Aviv 69978, Israel.

PMID: 26359206 PMCID: PMC4647855 DOI: 10.1038/ncomms9239

Abstract

The interface between the two band insulators SrTiO3 and LaAlO3 has the unexpected properties of a two-dimensional electron gas. It is even superconducting with a transition temperature, T(c), that can be tuned using gate bias V(g), which controls the number of electrons added or removed from the interface. The gate bias-temperature (V(g), T) phase diagram is characterized by a dome-shaped region where superconductivity occurs, that is, T(c) has a non-monotonic dependence on V(g), similar to many unconventional superconductors. Here, we report, the frequency of the quantum resistance-oscillations versus inverse magnetic field for various V(g). This frequency follows the same non-monotonic behaviour as T(c); a similar trend is seen in the low field limit of the Hall coefficient. We theoretically show that electronic correlations result in a non-monotonic population of the mobile band, which can account for the experimental behaviour of the normal transport properties and the superconducting dome.

References

  1. Phys Rev Lett. 2011 Apr 22;106(16):166807 - PubMed
  2. Phys Rev Lett. 2000 Sep 18;85(12):2565-8 - PubMed
  3. Phys Rev Lett. 2004 Sep 3;93(10):106803 - PubMed
  4. Nature. 2013 Oct 24;502(7472):528-31 - PubMed
  5. Phys Rev Lett. 2010 Nov 12;105(20):206401 - PubMed
  6. Phys Rev Lett. 2010 Mar 26;104(12):126802 - PubMed
  7. Phys Rev Lett. 2010 Mar 26;104(12):126803 - PubMed
  8. Nature. 2008 Dec 4;456(7222):624-7 - PubMed
  9. Phys Rev B Condens Matter. 1994 May 1;49(17):12095-12104 - PubMed
  10. Nature. 2004 Jan 29;427(6973):423-6 - PubMed
  11. Phys Rev Lett. 2009 Nov 27;103(22):226802 - PubMed
  12. Phys Rev Lett. 2014 Nov 21;113(21):216801 - PubMed
  13. Nat Commun. 2013;4:1838 - PubMed
  14. Nature. 2011 Jan 13;469(7329):189-93 - PubMed
  15. Nat Commun. 2012;3:1129 - PubMed
  16. Nat Commun. 2011;2:188 - PubMed
  17. Phys Rev Lett. 2015 Jul 3;115(1):016803 - PubMed
  18. Science. 2006 Sep 29;313(5795):1942-5 - PubMed
  19. Nat Commun. 2015 Jan 13;6:6028 - PubMed
  20. Phys Rev Lett. 2009 Apr 24;102(16):166804 - PubMed
  21. Phys Rev Lett. 1993 Mar 1;70(9):1311-1314 - PubMed

Publication Types