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Title: POTENTIAL%20APPLICATIONS%20OF%20SPINTRONICS


1
POTENTIAL APPLICATIONS OF SPINTRONICS
M.Cahay
February 4, 2005
  • Dept. of ECECS, Univ.of Cincinnati,
  • Cincinnati, Ohio 45221
  • http//www.ececs.uc.edu/mcahay


2
Outline
  • A Little quBit of History
  • Success Story Giant Magnetoresistance
  • Spin Valve
  • Requirements for spintronics
  • Zeeman, Spin-Orbit Effects
  • Injection, Manipulation, Detection
  • Magnetoresistive biosensors
  • Conclusions

3
Brief HistorySpintronics-Magnetoelectronics
  • Stern-Gerlach Experiment (Early 1920s)
  • spin concept 1920s
  • Pauli-Dirac Equation (Late 1920s)
  • 1980s Study of Mesoscopic systems
    Landauer-Buttiker Formalism
  • Breakdown of Moores Law?
  • 1988 Giant Magnetoresistance in Magnetic
    multilayers, magnetic read heads, magnetic
    sensors, spin valves.

4
Brief HistorySpintronics-Magnetoelectronics
  • 1990 SPINFET proposal by Datta and Das
  • 1990s Lots of work on Ferromagnet/ (metal,
    semiconductor, superconductor) interfaces.
  • DMS diluted magnetic semiconductors (ZnMnSe,
    GaMnAs,GaMnN,)
  • 1985 David Deutsch
  • Quantum Mechanical Turing Machine

5
Brief HistorySpintronics-Magnetoelectronics
  • 1995 P.Schors algorithm for fast factorization
    of large integers (cryptography)
  • 1997 L.K.Grovers search algorithm for efficient
    search of large database
  • 1990s Lots of proposal for implementation of
    qubits and quantum computers (NMR, Ion trap,
    quantum dot)
  • Search in Spintronics and Quantum Computing will
    continue to feed on each other

6
SIA ROADMAP - Moores Law
7
Requirements for Spintronic Integrated Circuits
  • Simple device structure for high degree
  • of integration and high process yield.
  • Large magnetocurrent for high speed operation
  • High transconductance for high speed operation
  • High amplification capability (V, I, and/or
    power)
  • Small power delay product and small off-current
  • for low power dissipation

8
Preliminaries Stoner Model
E(k)
Exchange Energy
k
Ferromagnetic Contact
9
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10
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11
GMR Read Head
12
RAM with GMR Elements
13
Preliminiaries Zeeman Effect
14
PreliminariesSpin-Orbit Interaction
15
Ferromagnet/Sm Interface
16
Contact Selection
  • Ferromagnetic contact (Fe, Ni, Co)
  • HMF candidates Heusler Materials
  • Dilute Magnetic Semiconductors (GaMnAs, ZnMnSe,
    ZnMnTe,GaMnN)
  • More recently, wide band gap ferromagnetic
    semiconductors and oxides
  • S.J. Pearson et al., Wide band gap
    ferromagnetic Semiconductors and oxides, Journal
    of Applied Physics, Vol.93, pp.1-13 (2003)

17
Ferromagnetic contact/semiconductor
interfacesHow good are they?
  • Why Ferromagnetic Contacts (Fe, Ni, Co)?
  • Because Curie Temperature Is Above Room
    Temperature!
  • Hence, devices could work at 300k.
  • FM are good source of spin polarized electron
    sources
  • (Stoner model)

Theoretical Predictions
  • Classical diffusion eq. predicts very small
    spin injection efficiency across Fe/Sm interface
    (G. Schmidt et al. PRB 62,R4790 (2000). Main
    reason Large conductivity mismatch between the
    two materials.
  • Not so fast! E.I.Rashba (Phys.Rev.B 62 R16267
    (2000)).
  • If you can adjust interface resistance by using
    a tunneling barrier, the situation can improved
    drastically!.

18
Ferromagnetic contact/semiconductor
interfacesHow good are they?
  • Rashba's prediction was confirmed
  • experimentally using
  • (a) Schottky barriers
  • H.J.Zhu et al., PRL 87, 016601 (2001) (Fe/GaAs),
    2 efficiency
  • A.T.Hanbicki et al, APL 80, 1240 (2002)
  • A.T.Hanbicki et al, APL 82, 4092 (2003),
    (Fe/AlGaAs), 33 efficiency
  • (b) Thin Metal Oxides
  • V.F. Motsynyi et al, APL 81, 265 (2002)
  • T. Manago and H. Akinaga, APL 81, 694 (2002)
  • (c) AlAs barriers
  • S.H.Chun et al, PRB 66, R100408 (2002).

19
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20
Spin Relaxation Mechanisms
  • The Elliot-Yafet Scattering Mechanism
  • As a result of the SO-contribution to the crystal
  • Hamiltonian, conduction-band states of some
  • semiconductors are not spin eigenstates. This
    leads to
  • the possibility for spin-flip scattering even for
    spin
  • independent impurity scattering (due to Coulombic
  • scattering for instance).
  • For the same reason, spin-independent
    electron-electron
  • scattering can also cause spin-flip transitions

21
DYAKONOV-PERELSPIN RELAXATION IN A QUANTUM WIRE
  • DRESSELHAUS HAMILTONIAN
  • RASHBA HAMILTONIAN

x
z
x
y
22
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23
RAMSAUER (FABRY-PERROT) RESONANCES
24
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25
ONE REPULSIVE IMP. 300 angs from left
contact INFLUENCE OF SCATTERING STRENGTH
26
Magnetoresistive-Based BiosensorsD.L.Graham et
al, Trends in biotechnology vol.22, 455 (2004)
27
Conclusions
  • Spintronics has already some success stories!
  • (giant magnetoresistance/spin valve)
  • Quantum Computing Too early to tell!
  • Other potential Spintronics organics,
  • Spintronics Biosensors, Magnetic Sensors.
  • Want to know more about it? Buy the book
  • Introduction to Spintronics.in 2006.
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