Functionalization of multiferroic oxide structures for spintronic devices

We study the electronic and magneto-transport properties of multiferroic oxide-based structures and explore their potential for spintronic applications. In particular, we point out the possibility of using the two dimensional electron gas (2DEG) formed at the interface of helimagnetic oxides as a spin-field-effect transistor and a flash memory device. The operation of this device relies on the fact that the topology of the multiferroic oxide local magnetic moments results in a resonant momentum-dependent effective spin-orbit interaction acting on 2DEG. The spin polarization dephasing is strongly suppressed which is crucial for functionality. The effective spin-orbit interaction and the carrier spin precession phase depend linearly on the magnetic spiral helicity which, due to the magnetoelectric coupling, is electrically controllable. We also consider helical multiferroic tunnel junctions with a normal metallic layer as the bottom electrode and a ferromagnetic layer as the other electrode. It is shown that the tunnel-magneto-resistance is spatially dependent and is controllable via an external electric field.

[1]  S. Datta,et al.  Electronic analog of the electro‐optic modulator , 1990 .

[2]  C. Ahn,et al.  Electric field effect in correlated oxide systems , 2003, Nature.

[3]  C. L. Zhang,et al.  Ferroelectricity in an s=1/2 chain cuprate. , 2007, Physical review letters.

[4]  D. Awschalom,et al.  Emergence of the persistent spin helix in semiconductor quantum wells , 2009, Nature.

[5]  Y. Tokura,et al.  Ferroelectricity and giant magnetocapacitance in perovskite rare-earth manganites. , 2004, Physical review letters.

[6]  Y. Pershin Long-Lived Spin Coherence States in Semiconductor Heterostructures , 2003, cond-mat/0311223.

[7]  Robert Karplus,et al.  Hall Effect in Ferromagnetics , 1954 .

[8]  X. Cartoixà,et al.  A resonant spin lifetime transistor , 2003 .

[9]  E. Rashba,et al.  Oscillatory effects and the magnetic susceptibility of carriers in inversion layers , 1984 .

[10]  Topological Hall effect and Berry phase in magnetic nanostructures. , 2003, Physical review letters.

[11]  Y. Tokura,et al.  Rotation of an electric polarization vector by rotating magnetic field in cycloidal magnet Eu0.55Y0.45MnO3. , 2008, Physical review letters.

[12]  J. Berakdar,et al.  Tunneling anisotropic magnetoresistance of helimagnet tunnel junctions , 2010, 1002.0221.

[13]  Jeremy Levy,et al.  Oxide Nanoelectronics on Demand , 2009, Science.

[14]  J. Berakdar,et al.  Multiferroic oxides-based flash memory and spin-field-effect transistor , 2009, 0906.4210.

[15]  Peeters,et al.  Two-dimensional electrons in lateral magnetic superlattices. , 1995, Physical review. B, Condensed matter.

[16]  W Wegscheider,et al.  Tunneling anisotropic magnetoresistance and spin-orbit coupling in Fe/GaAs/Au tunnel junctions. , 2007, Physical review letters.

[17]  J. Berakdar,et al.  Electrically controlled persistent spin currents at the interface of multiferroic oxides , 2009, 0907.3023.

[18]  J. Schliemann,et al.  Nonballistic spin-field-effect transistor. , 2002, Physical review letters.

[19]  A. Millis,et al.  Two-Dimensional Electron Gases at Oxide Interfaces , 2008 .

[20]  Marc Cahay,et al.  Reexamination of some spintronic field-effect device concepts , 2004 .

[21]  G. Dresselhaus Spin-Orbit Coupling Effects in Zinc Blende Structures , 1955 .