future materials research in data storage nsf workshop on cyberinfrastructure for materials science...
TRANSCRIPT
Future Materials Research in Data Storage
NSF Workshop on Cyberinfrastructure for Materials Science
Mark H. KryderCTO and Sr. Vice President, Research, Seagate TechnologyUniversity Professor, Carnegie Mellon University
Mark H. KryderNSF Workshop 08-06 Page 2
Outline
Recording Overview
Materials Problems in Future Recording Technologies
Perpendicular Recording
Heat Assisted Magnetic Recording
Bit Patterned Media
TGMR/GMR Readers
Multiferroics
Discussion of Modeling Needs
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Disc Drives Today Cover the Widest Range of Users and Systems Ever
Handheld Gaming DVR Notebook Desktop Enterprise
12 GB12 GB 750 GB750 GB 160 GB160 GB 73 GB73 GB 300 GB300 GB750 GB750 GB 750 GB750 GB
Low-cost, high-capcity, disk drives are enabling new devices, resulting in rapid growth of the storage industry and the emergence of new industries. e.g. Apple iPod, PVR’s, X-Box, automobile navigation systems, digital video cameras, etc.
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Areal Density Growth
0.1
1
10
100
1000
10000
100000
year
gig
ab
it / in2
Single particle superparamagnetic limit (estimated)
Charap’s limit (broken)
• Late 1990s – super paramagnetic limit demonstrated through modeling
• Longitudinal recording reaching areal density limits
• Perpendicular expected to extend to 0.5-1 Tb/in2
• Additional innovations required at that point• heat-assisted
recording (HAMR)• bit patterned
media (BPM) recording
• Areal Density CAGR 40%
• Transfer Rate CAGR 20%
Perpendicular
HAMR
HAMR+BPM
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Magnetic domains oriented in the direction of travel of the head.
Longitudinal Recording
Perpendicular Recording
Soft underlayer “mirrors” write head and makes it possible to write domains much closer together.
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Magnetic Media EvolutionMagnetic Media Evolution
0
0.05
0.1
0.15
0.2
0.25
0 5 10 15 20 25 30 35
grain size (nm)
no
rmal
ized
fre
qu
ency
24 Gbit/in2
10 nm mean size
16 Gbit/in2
11 nm mean size
10 Gbit/in2
12 nm mean size
6 Gbit/in2
15 nm mean size
100 Gbit/in2
9.1 nm mean sizeStd. Dev. 1.7nm
45 Gbit/in2
9 nm mean sizeStd. Dev. 2.2nm
20nm20nm20nm
Physical grain size below 10 nm
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HAMR can theoretically extend areal density beyond 10 Tbpsi
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YCo5
HAMR Potential Ability to record on media
with anisotropy beyond writability with current perpendicular recording technology
Increased resolution with cross- and in-track thermal gradient recording
HAMR freezing dynamics allowing more intergranular exchange and unique composite media designs.
10× AD gain potential with FePt
10 n
m
Dieter Weller
SmCo5
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HAMR Head Disc Interface Material Needs• Media Overcoat (< 2 nm) and Lubricant must be able to
withstand the repeated exposure to the high writing temperature.
• New media overcoat materials will be needed.
• Carbon overcoat can be damaged and/or graphitized at much lower temperature than its 560°C oxidation temperature.
• New Disc Lubricant materials will be required.
120mJ/cm2
Media DLC is removed
0 100 200 300 400 500 600 700 800 900
0
20
40
60
80
100
We
igh
t (%
)
Temperature (Degree C)
Zdol 2000 Lubricant 1 Lubricant 2
In Air10 K/min heating rate
0.0
1.0
2.0
3.0
4.0
5.0
400 500 600 700 800
Curie Temperature (K)
Ani
sotr
opy
(10^
7 er
g/cc
)
HDI
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Bit Patterned MediaLithography vs. Self Organization
Lithographically Defined
Major obstacle is finding low cost means of making media• At 1 Tbpsi, assuming a square bit cell and
equal lines and spaces, 12.5 nm lithography would be required
• Semiconductor Industry Association roadmap does not provide such linewidths within the next decade
Direct E-Beam Write or Di-Block Co-Polymer
Idea:Use Pattern Assisted Assembly to establish circumferential tracks on discs
FePt Self-Organizing Media
130 nm
6 nm FePt particles
“9 Tb/in2“
~mm
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Di-Block Co-polymer Template
A B
Lo
Guiding patterns can provide long
range order
• controlled 2D alignment to guiding patterns
• balance polymer-interface vs polymer-substrate interactions
Block-copolymers form naturally ordered nano-structures
A-B block copolymerprecursorsubstrate
• control of vertical orientation on any substrate• improve long-range order and uniformity• selective removability of one component• reduce L0 without losing uniformity, order• use of “environmentally safe” chemicals
Use as a template for pattern transfer• additive process (fill in holes by plating):
- ensure open contact to metal substrate- ensure all pores get filled equally
• subtractive process (transfer down by RIE):- etching requires high etch-resistive resist
lines dots
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Examples of some h=20nm h=10nm
Uniaxial Ferromagnetic Materials Cube Sphere Cylinder Cylinder
Kux107 Ms Tc Hk Vp Dp Dp Dp Dp
Material (ergs/cc) (emu/cc) (K) (kOe) (nm3) (nm) (nm) (nm) (nm)
Co hcp alloy
CoCrPt 0.3 330 18.2 966 9.9 12.3 7.8 11.1
Co3Pt 2 1100 36.4 145 5.3 6.5 3.0 4.3
CoPt3 0.5 300 600 33.3 580 8.3 10.3 6.1 8.6
Co 0.45 1422 1393 6.3 644 8.6 10.7 6.4 9.1
Multilayer #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0!
Co2/Pt9 1 360 500 55.6 290 6.6 8.2 4.3 6.1
Co2/Pd9 0.6 360 500 33.3 483 7.8 9.7 5.5 7.8
L10 #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0!
FePd 1.8 1100 760 32.7 161 5.4 6.7 3.2 4.5
FePt 6.6 1140 750 115.8 44 3.5 4.4 1.7 2.4
CoPt 4.9 800 840 122.5 59 3.9 4.8 1.9 2.7
Rare Earth #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0! #DIV/0!
Fe14Nd2B 4.6 1270 585 72.4 63 4.0 4.9 2.0 2.8
SmCo5 20 910 1000 439.6 14 2.4 3.0 1.0 1.4
Self Organized Magnetic Array Media
Important Research Topics:• Particle Size and Distribution Control• Eliminate Sintering / Coarsening during anneal e.g. FCC-FCT (A1 – L10) Phase Transformation • Magnetic Easy Axis Orientation • Registered Large Scale Assembly• Packing density• Tribology
Dp: smallest possible thermally stable magnetic grain core size!
S. Sun, Ch. Murray, D. Weller, L. Folks, A. Moser, Science 287, 1989 (2000).
Solvent Evaporation
130 nm
e.g. 6 nm FePt particles
1 particle/bit~“9 Tb/in2“
~m
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TGMR/GMR Reader Materials
To
p S
hie
ld
Magnet MagnetFL
AFM/SAF/RL
Bottom ShieldInsulator
CurrentFlow
ElectronFlow
FL
RL
TunnelingBarrier
Flux from the media rotates reader free layer magnetization thus changing spin polarized electron tunneling conduction.
MediaField
OutputVoltage
FL-RL
FL-RL
FL
LinearRange
Operate in the linear range of transfer function.
Sensitivity (slope)is determined by TMR
Alternate Barrier TGMR (MgO)
Improved amplitude, and lower RA
Potential to extend TGMR reader to area density
Current problem – Maintaining soft magnetic property of free layer, while keeping high DR/R and low RA.
CCP Design (current confined path)
A discontinuous oxide buried in metal
Higher DR/R and RA as compared to CPP Spin Value
Potential to use for area density of 400~ 600Gb/In2.
Current problem – Reducing variation of RA, and DR/R, and increasing DR/R.
CPP Spin Valve With Metal or Half Metal Spacer
Could offer better reliability, and SNR at very high KTPI
Potential to use for area density of 600Gb/In2 and behind
Current problem – Concept not proven, and processing half metals at temperature magnetic head can tolerate difficult
AFMPinned Layer
RuRef. Layer
Free Layer
AFMPinned Layer
RuRef. Layer
CuFree Layer
AFMPinned Layer
RuRef. Layer
MgOFree Layer
Reader Development Approaches
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Multiferroic Data Storage System Readback is difficult from PE media, due to free charges, but not from FM media.
Generating enough magnetic field to write to thermally stable FM media is difficult.
An electric field can be used to assist writing by by using a media that is both PE and FM (Multiferroic). The data could then be read back using an MR head.
Both single phase and multiferroic materials exist, but composite materials are most interesting due to their higher transition temperatures (both PE & FM above RT).
• A composite material is achieved by combining MS and PE materials [ex. BiFeO3-CoFe2O4 or BaTiO3-CoFe2O4]. An electric field applied to the composite will induce strain in the PE constituent which is passed along to the MS constituent, where it induces a change in the magnetic anisotropy.
V+
V-
V+
V-
I
Diagram of an Example Recording System
P PM
P PM
P PM
P PM
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Computing Needs in Magnetic Recording Technology
Micromagnetic models of media structure with 3-10 nm grain size and variable exchange coupling at the grain boundaries that allow us to understand the recording of 10’s to 1000’s of bits involving 50-100 grains each.
Models which enable prediction of magnetic materials properties and processes for making them that enable growth of materials with variable grain sizes, variable magnetic parameters, and variable exchange coupling across grain boundaries.
Models of tribological properties of thin film (<2 nm) materials. Models of self organization in diblock copolymers and in magnetic
nanoparticle arrays. Predictions of improved giant and tunneling magnetoresistive
materials. Predictions and understanding of multiferroic materials. NUMEROUS OTHERS!!