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The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

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Page 1: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

The Story of Giant Magnetoresistance (GMR)

From Laboratory to Hard Drive

Anne Reilly

Grants Development UHCL

Adjunct Professor of Physics

Page 2: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

The Nobel Prize in Physics 2007

The Nobel Prize in Physics is awarded to ALBERT FERT and PETER GRÜNBERG for their discovery of Giant Magnetoresistance. Applications of this phenomenon have revolutionized techniques for retrieving data from hard disks. The discovery also plays a major role in various magnetic sensors as well as for the development of a new generation of electronics. The use of Giant Magnetoresistance can be regarded as one of the first major applications of nanotechnology.

Fert Grunberg

Page 3: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Outline

1. Magnetic Materials: Basic Propertiesa. Source of Magnetismb. Types of Magnetismc. Domains and Hysteresisd. Spin-Dependent Transport

2. The Discovery of Giant Magnetoresistancea. Atomically Engineered Structuresb. Fe/Cr Multilayers and Antiferromagnetic Couplingc. Giant Magnetoresistanced. Advances to Applications

3. GMR and the Computer Hard Drive

Page 4: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Magnetic Materials:Basic Properties

Page 5: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Source of Magnetism: Moving Electric Charge (Current)

www.lanl.gov

Page 6: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Source of Magnetism: Moving Electric Charge (Current)

Page 7: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Source of Magnetism: Moving Electric Charge (Current)

Atomic Magnetism arises from electron angular momentum and spin

ML

I

vL

r

e-

S

Page 8: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Source of Magnetism: Moving Electric Charge (Current)

Atomic Magnetism arises from electron angular momentum and spin

Atomic magnetic moment: SgL BeB

M

Angular momentum vector Spin vector

Gyromagnetic ratio ge~ 2

Bohr magneton

m

eB 2

ML

I

vL

r

e-

S

Page 9: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

What happens in a solid?Individual atomic moments in solids are usually not aligned.

BM

Page 10: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

What happens in a solid?Individual atomic moments in solids are usually not aligned.

DiamagnetismInduced moment is opposite of external field, B(Mdia is very small, except in superconductors)

ParamagnetismInduced moment is in same direction as field

BM

M

M

B

B

Page 11: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Ferromagnetism (3d and rare earth elements)

Occurs in materials we usually call ‘magnetic”. Interaction between electrons (exchange) causes moments to align spontaneously.

M

Page 12: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

•Central for understanding magnetic interactions in solids•A quantum mechanical effect, arises from Coulomb electrostatic interaction and the Pauli exclusion principle

Coulomb repulsionenergy high

Coulomb repulsionenergy lowered

(105 K !)Jr

eUC

182

0

2

10~4

Exchange Interaction

Page 13: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Natural Principle: Minimization of Energy

Page 14: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

+

1 2

Ze

e- e-

Exchange Interaction: A Quantum Mechanical Effect

H

E

jiex SSJ 2H

J>0

J<0

Page 15: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

In ferromagnetic materials, exchange interaction leads to an alignment of atomic spins.

However, this leads to a large external and dipolar magnetic fields which will tend to demagnetize the material. Domains are formed to minimize this effect.

From http://www.aacg.bham.ac.uk/magnetic_materials

Domains

Domain wall

Page 16: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Hysteresis = Magnetic Memory

M

B

B

B

Ni thin film

Page 17: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Spin-Dependent Transport and Ordinary (Anisotropic) Magnetoresistance (AMR)

Discovered by Lord Kelvin in 1856.

V = IRI

B

www.emg.tu-bs.de

AMR~1-2%

Page 18: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Spin Dependent ScatteringResistance (R) and Resistivity ( determined by scattering of electrons. In ferromagnets, because of the exchange interaction, one spin state is favored. This means that there are less energy states available for one spin than the other, and:

in ferromagnetic element metals

Ene

rgy

Density of StatesN(E)

Ene

rgy

Density of StatesN(E)

EF

Fermi Level

(s-band) (d-band)

Page 19: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Spin Dependent ScatteringResistance (R) and Resistivity ( determined by scattering of electrons. In ferromagnets, because of the exchange interaction, one spin state is favored. This means that there are less energy states available for one spin than the other, and:

in ferromagnetic element metals

www.nobelprize.org

Page 20: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

The Discovery of Giant Magnetoresistance

Page 21: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Nanotechnology

“Atomically engineered structures”

substrate

Material 1

Material 2

3.5nm Co / 0.65 nm W

The 1980’s necessary technological advance:

http://www.mats-uk.com/applications/magnetic.html

Page 22: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Physics.umn.edu

Molecular Beam Epitaxy (MBE)

also, Sputtering

Page 23: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Peter Grunberg et al., Discovery of AF coupling in Fe/Cr multilayers

www.cnrs.fr

“Layered Magnetic Structures: Evidence for Antiferromagnetic Coupling of Fe Layers across Cr Interlayers”, Physical Review Letters, 57, 2442–2445 (1986)

Page 24: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

www.nobelprize.org

(Fert) (Grunberg)

Phys. Rev. Lett. 61, 2472 (1988); Physical Review B 39, 4282 (1989)

Page 25: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Stuart Parkin and IBM:Understanding and Maximizing Effect for Application

nytimes.com

Page 26: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Major Step: Invention of Spin Valve

rug.nlDieny, Parkin (IBM)

Page 27: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Major Step: Current Perpendicular to the Plane (CPP) GMR

Zdnet.com

Jack Bass, William Pratt, Peter SchroederMichigan State University

Page 28: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Source of GMR: Spin Dependent Scattering

in ferromagnetic element metals

R high

F F FN N

R low

F F FN N

Anti-Parallel (AP)

Parallel (P)

Page 29: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Applications: Computer Hard Drive Read Sensors

Page 30: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

How your hard drive stores data

With more sensitive sensors,

bits can get smaller = higher storage density

01

0

Binary codeU 01010101H 01001000C 01000011L 01001100

Page 31: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

How your hard drive stores data

www.dmphotonics.com

High resolution MFM image of Seagate Barracuda 750Gb Hard Drive, ST3750640AS

Page 32: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Evolution of the Hard Drive

Page 33: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Evolution of the Hard Drive

IBM 305 RAMAC, 1956

4.4 MB = 50 24-inch diameter disks.

Leased $3200 month

Page 34: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

Evolution of the Hard Drive

2004: GB on the size of a quarter!

Page 35: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

http://nobelprize.org/mediaplayer/index.php?id=797

http://www.research.ibm.com/research/gmr.html

Links to See:

Page 36: The Story of Giant Magnetoresistance (GMR) From Laboratory to Hard Drive Anne Reilly Grants Development UHCL Adjunct Professor of Physics

The End… Questions?