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The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
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The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
Spin transfer (J
Spin transfer (J
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
Spintronics with semiconductors
Spintronics with semiconductors
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
Window only for lsf(N) > L
Window only for lsf(N) > L
e?V ? 1 meV
e?V ? 1 meV
from Jaffr
from Jaffr
The present and future of Spintronics
The present and future of Spintronics
Diffusive transport Ballistic transport
Diffusive transport Ballistic transport
Diffusive transport Ballistic transport
Diffusive transport Ballistic transport
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
The present and future of Spintronics
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The present and future of Spintronics

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1The present and future of Spintronics. 35(FS). GaMnAs (Tc?170K) and R.T. FS
In classical spintronics: new types of Electrical control of ferromagnetism TMR,
MTJ. Zagreb, May 2008, A. Fert, TAMR, spin transfer (GaMnAs) Field-induced
CNRS/Thales, Palaiseau, and Universit? metal/insulator transition. Example: spin
Paris-Sud. Tulapurkar et al. Hruska et al. injection from Fe into LED (Mostnyi et al,
2Introduction : Spin dependent PR. B 68, 2003).
conduction in ferromagnetic conductors, 36
Giant Magnetoresistance (GMR), Tunnel 37Nonmagnetic lateral channel between
Magnetoresistance (TMR). spin-polarized source and drain.
3 Semiconductor channel: « Measured effects
4? = ??/?? of the order of 0.1-1% have been reported
5 for the change in voltage or resistance
6 (between P and AP)…. », from the review
7 article « Electrical Spin Injection and
8 Transport in Semiconductors » by BT Jonker
9 and ME Flatt? in Nanomagnetism (ed.: DL
10 Mills and JAC Bland, Elsevier 2006).
11 38
12 39
13 40
14 41
15 42
16Spin Transfer (magnetic switching, 43
microwave generation) Spintronics with 44
semiconductors Spintronics with molecules. 45
17 46
18 47Window only for lsf(N) > L.
19 48e?V ? 1 meV. LSMO/CNT/LSMO: higher
20 voltage experiments thanks to large
21 interface resistances and small V2/R
22 heating at large V. Usual conditions:
23Spin transfer (J. Slonczewski, JMMM small bias voltage experiments. Uc=e2/2C.
1996, L. Berger, PR B 1996). Oscillatory variation of the conductance,
24 different signs of theMR depending on the
25 bias voltage and from sample to sample.
26Py = permalloy. Quasi-continuous DOS, same conditions as
27 for semiconductor or metallic channel.
28 49from Jaffr?s and A.F. (see also Yu and
29 Flatt?).
30 50
31 51
32 52Diffusive transport Ballistic
33 transport. + additional geometrical
34Spintronics with semiconductors and parameters when the number of conduction
molecules. channels is different for the injection
35Spintronics with semiconductors. and in the channel (W ? w in the example).
Magnetic metal/semiconductor hybrid 53
structures. Ferromagnetic semiconductors
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