zagreb, may 2008, a. fert, cnrs/thales, palaiseau, and université paris-sud

53
Zagreb, May 2008, A. Fert, CNRS/Thales, Palaiseau, and Université Paris- Sud In classical spintronics: new types of MTJ Spin transfer: switching, oscillators, synchronization -1.0 -0.5 0.0 0.5 1.0 -0.1 0.0 0.1 -1.0 -0.5 0.0 0.5 1.0 AP P m single- electron devices semiconductor s Spintronics with molecules Spintronics with The present and future of Spintronics Tulapurkar et al Hruska et al

Upload: serina-stephenson

Post on 02-Jan-2016

29 views

Category:

Documents


0 download

DESCRIPTION

Spin transfer: switching, oscillators, synchronization. AP. m. P. Spintronics with. Spintronics with. single-electron devices. semiconductors. molecules. Zagreb, May 2008, A. Fert, CNRS/Thales, Palaiseau, and Université Paris-Sud. In classical spintronics: new types of MTJ. - PowerPoint PPT Presentation

TRANSCRIPT

  • Zagreb, May 2008, A. Fert, CNRS/Thales, Palaiseau, and Universit Paris-SudIn classical spintronics: new types of MTJThe present and future ofSpintronics Tulapurkar et alHruska et al

  • Introduction :Spin dependent conduction in ferromagnetic conductors,Giant Magnetoresistance (GMR),Tunnel Magnetoresistance (TMR)

  • = /

  • Spin Transfer (magnetic switching, microwave generation)

    Spintronics with semiconductors

    Spintronics with molecules

  • Spin transfer (J. Slonczewski, JMMM 1996, L. Berger, PR B 1996)

  • Py = permalloy

  • Spintronics with semiconductors and molecules

  • GaMnAs (Tc170K) and R.T. FS Electrical control of ferromagnetism TMR, TAMR, spin transfer (GaMnAs)Field-induced metal/insulator transitionSpintronics with semiconductors Magnetic metal/semiconductor hybrid structures Example: spin injection from Fe into LED (Mostnyi et al, PR. B 68, 2003)Ferromagnetic semiconductors (FS)

  • Nonmagnetic lateral channel between spin-polarized source and drainSemiconductor channel:Measured effects of the order of 0.1-1% have been reported for the change in voltage or resistance (between P and AP)., from the review article Electrical Spin Injection and Transport in Semiconductors by BT Jonkerand ME Flattin Nanomagnetism (ed.: DL Mills and JAC Bland, Elsevier 2006)

  • Window only for lsf(N) > L

  • Quasi-continuous DOS, same conditions as for semiconductor or metallic channelUc=e2/2CeV 1 meVUsual conditions: small bias voltage experimentsLSMO/CNT/LSMO: higher voltage experiments thanks to large interface resistances and small V2/R heating at large VOscillatory variation of the conductance, different signs of theMR depending on the bias voltage and from sample to sample

  • from Jaffrs and A.F.(see also Yu and Flatt)

  • Diffusive transport Ballistic transport+ additional geometrical parameters when the number of conduction channels is different for the injection and in the channel (W w in the example)