Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Prediction of a spin-polarized two-dimensional electron gas at the LaAlO3/EuO(001) interface

Yong Wang, Manish K. Niranjan, J. D. Burton, Joonhee M. An, Kirill D. Belashchenko, and Evgeny Y. Tsymbal
Phys. Rev. B 79, 212408 – Published 23 June 2009

Abstract

First-principles calculations predict the existence of a spin-polarized two-dimensional electron gas (2DEG) at the LaO/EuO interface in a LaAlO3/EuO(001) heterostructure. This polar interface favors electron doping into the Eu-5d conduction bands resulting in a 2DEG formed at the interface. Due to the exchange splitting of the Eu-5d states, the 2DEG is spin polarized below the Curie temperature of EuO. The predicted mechanism for the formation of a spin-polarized 2DEG at the interface between polar and ferromagnetic insulators may provide a robust magnetism of the 2DEG which is interesting for spintronics applications.

  • Figure
  • Figure
  • Figure
  • Figure
  • Received 27 March 2009

DOI:https://doi.org/10.1103/PhysRevB.79.212408

©2009 American Physical Society

Authors & Affiliations

Yong Wang, Manish K. Niranjan, J. D. Burton, Joonhee M. An, Kirill D. Belashchenko, and Evgeny Y. Tsymbal*

  • Department of Physics and Astronomy, Nebraska Center for Materials and Nanoscience, University of Nebraska, Lincoln, Nebraska 68588, USA

  • *tsymbal@unl.edu

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 79, Iss. 21 — 1 June 2009

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1
    (Color online) Atomic structure of the LaO/EuO interface in the (LaAlO3)8.5/(EuO)15(001) superlattice containing 8.5 unit cells of LaAlO3 and 15 monolayers of EuO within the supercell. Indices l and m denote atomic monolayers and are increasing with separation from the interface. l=8 in EuO and m=9 in LaAlO3 correspond to the middle of the respective layers.Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) Atomic displacements in the (LaAlO3)8.5/(EuO)15(001) superlattice with respect to the atomic “bulk” positions. The latter are determined by fixing the in-plane lattice constant and optimizing the interlayer distance, as described in the text. The vertical dashed lines indicate interfaces.Reuse & Permissions
  • Figure 3
    Figure 3
    (Color online) Layer- and spin-resolved DOS on (a) EuO, (b) LaO, and (c) AlO2 monolayers located at different planes l and m away from the LaO/EuO interface (as labeled in Fig. 1). Top (bottom) panels show the majority (minority) spin. In panel (a), the majority-spin states at energies below 1eV are the occupied Eu-4f states. The vertical lines denote the Fermi energy (EF).Reuse & Permissions
  • Figure 4
    Figure 4
    (Color online) Spin-dependent charge distribution across the (LaAlO3)8.5/(EuO)15(001) supercell. The notation for the atomic layers is the same as in Fig. 1. The dashed lines indicate interfaces.Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×