The Future of Magnetic Recording Technology April 11, 2008 Richard New Director of Research © 2008 Hitachi Global Storage Technologies Agenda Overview of Hitachi GST & San Jose Research Center Technology Challenges for Magnetic Recording Future Recording Directions Patterned Media Thermally Assisted Recording © 2008 Hitachi Global Storage Technologies 4/11/2008 2 Hitachi Ltd. Overview Revenue US$ 86,847 million Operating Income US$ 1,547 million Number of Employees 384,444 Consolidated Subsidiaries 934 Consolidated figures for FY 2006, ended March, 2007 Information & Telecommunication Systems Power & Industrial Systems 24% Financial Services 5% 12% Logistics, Services and Others High Functional Materials © 2008 Hitachi Global Storage Technologies 13% US$ 86.8 billion 29% 日立の事業 18% Electronic Devices 15% Digital Media & Consumer Products 4/11/2008 3 Hitachi Global Storage Technologies Overview Hitachi Global Storage Technologies (GST) was formed when Hitachi Ltd. purchased the Storage Technology Division from IBM. The hard disk drive operations from IBM and Hitachi Ltd. were combined and launched as a new company on January 1, 2003. Revenues in 2006 of $4.9 billion, 33K employees worldwide. US headquarters in San Jose, California. WW operations in 9 countries (R&D in US & Japan, manufacturing in China, Phillipines, Thailand, Singapore, Japan and US). 1.5K R&D employees, with industry’s largest patent portfolio. Enterprise 3.5-inch 2.5-inch √ √ √ √ √ √ √ √ √ √ √ √ © 2008 Hitachi Global Storage Technologies √ 4/11/2008 4 Hitachi GST Headquarters in San Jose, CA © 2008 Hitachi Global Storage Technologies 4/11/2008 5 Hitachi San Jose Research Center : Our People San Jose Research Center Staff Technical Disciplines ~100 permanent research staff >70% hold PhD degree Geographically diverse 50% NA; 25% EMEA; 25% Asia 15 Fellows of professional societies Wide range of technical disciplines Educational Institution Educational Institution 10 9 8 7 6 5 4 3 2 1 UC St an f or d UC Be SD rk el ey UC LA Sa n Ca l Jo t e se ch St at e CM Ill U in o G Co is eo rg rn e ll ia Te c Ha h rv ar R d Un W T M iv H I Un er s Aa T iv it y che er o si f B n ty a of se To l ky o 0 © 2008 Hitachi Global Storage Technologies 4/11/2008 6 Hitachi San Jose Research Center : Our Facilities Expose / Develop Plating / Etching Resist Apply / Strip / Bake San Jose Research Center Facilities 58,000 sq ft of lab space 15,000 sq ft of clean room space Recording head prototyping line Full nano-fabrication facility E-beam, optical litho, deposition, RIE, mill, characterization, SEM. MEMS lab, model making / machining shop © 2008 Hitachi Global Storage Technologies CMP Vacuum E-beam Photo MEMS 4/11/2008 7 Agenda Overview of Hitachi GST & San Jose Research Center Technology Challenges for Magnetic Recording Future Recording Directions Patterned Media Thermally Assisted Recording © 2008 Hitachi Global Storage Technologies 4/11/2008 8 Areal Density Trend 10000 Hitachi/HGST 20~60% CGR Areal Density (Gb/in2) IBM/HGST 1000 Quantum/Seagate 60% CGR Toshiba GMR heads MEPRML channel etc. Fujitsu 100 Samsung 90% CGR 10 1 MR head thin film m edia PRML channel etc. 25% CGR AFC-LMR TMR Advanced PMR? DTM BPM TAR PMR TFC etc. CPP-GMR 60% CGR 0.1 1990 1995 2000 2005 2010 2015 Year product available (mobile) © 2008 Hitachi Global Storage Technologies 4/11/2008 9 HDD Technology Challenges Head/Disk Spacing Recording System Requirements: Center the recording head above the data track. Fly the head very close to the recording medium. Magnetic Element Servo Mechanics Data TMR Write Head Magnetic Spacing Physical Spacing Magnetic Overcoat Film Disk Substrate Data Servo Servo Servo Write sharp transitions in the recording medium. Store the data reliably for more than 10 years. Read the data back with high SNR and high resolution. Decode the signal with very few readback errors (~10-11 Sector Failure Rate). All with high reliability, high performance, low power, and for pennies per GB. © 2008 Hitachi Global Storage Technologies 01010100101101 10101010101010 01010101110101 10101101010010 01010101010101 I Disk Signal Processing Read Head 4/11/2008 10 Servo Mechanics Challenges FDB Motors Airflow Modeling 1000 kTPI Æ Track pitch = 25 nm Æ NRRO Sigma = 0.6 nm 1000 Large TPI jump with BPM kTPI • Reduce Disturbances – Motor Vibration – Airflow Management • Increase Disturbance Rejection – Increased Mechanical BW – External Vibration Feed Forward – Adaptive Servo Algorithms – Dual Stage Actuation (milli or micro−actuator) • Shock Resilience 25% TPI CAGR Patterned Media Continuous Media 100 2005 2006 2007 2008 2009 2010 2011 2012 2013 Year Micro Actuator Suspension Slider Microactuator G Shock Recording Head © 2008 Hitachi Global Storage Technologies 4/11/2008 11 Magnetic Spacing Challenges 1000 Design Constraint(s) Recession Slider Process Slider Overcoat Scratch resistance Clearance Lube Transfer Take Off Height Disk Roughness Lubricant Scratch resistance Media Overcoat Corrosion, Scratch resistance Mag Spacing (nm) Magnetic Spacing Component 10 1 0.1 Surface Topology & Overcoats Magnetic Element 100 1 10 100 Areal Density (Gb/in2 ) 1000 Thermal Fly Height Control Slider Recession Slider Overcoat Lube Magnetic Spacing Clearance TOH Media Overcoat Magnetic Film Disk Substrate © 2008 Hitachi Global Storage Technologies 4/11/2008 12 The Recording Mechanism Write Head Current Read Head Write Flux Magnetization into the plane Magnetization out of the plane Disk Rotates This Way Track Width Hard Magnetic Recording Layer (CoCrX granular alloy) Fly Height Exchange Break Layer Soft Underlayer Old Data New Data Media Top View Skew Angle Read Width Pole Tip 1 0 111 0 0 1 1 0 1 0 0 0 0 1 0 0 11 0 Readback Signal Voltagel © 2008 Hitachi Global Storage Technologies Write Width Detected Data time 4/11/2008 13 Writeability, Thermal Stability, and SNR Magnetic Grain Single Grain Magnetostatic Energy CONVENTIONAL MEDIA 50 50 nm nm Energy Barrier -90 0 90 Magnetization Angle Magnetic Stability: energy barrier Problem: thermal energy ∝ • To increase SNR, need small grains. • Smaller grains are thermally unstable. • To avoid thermal instability, increase grain anisotropy Ku. • This increases the medium coercivity and makes the medium difficult to write. © 2008 Hitachi Global Storage Technologies anisotropy x volume kB x temperature = K uV k BT Solutions: • Capped and exchange spring media. • Work with larger ‘grains’: patterned media. • Work with higher anisotropy: thermally assisted recording (TAR). 4/11/2008 14 Media Technology History of Media Innovations Media Technology Challenges • Thin film media (early 1990’s) • Reduce grain size (8-9nm -> 6-7 nm). • Increase anisotropy (to maintain stability). • Maintain high quality growth: – Uniform grain size – Narrow switching field distributions. • Reduce media layer thicknesses: – Reduce head to media spacing – Reduce head to SUL spacing • AFC longitudinal media (pixie dust) (2000) • PMR capped media (2005) • Exchange spring media (2008) Capped Media Exchange Spring Layer (ESL) Media Soft Cap Layer Soft Cap Layer Mag Layer Coupling Layer Mag Layer Media Stack Mag Layer Granular Structure COC Mag Layers H=0 H H H Underlayer Seed Layer Soft Underlayer (SUL) Exchange Break Layer (EBL) Adhesion Substrate © 2008 Hitachi Global Storage Technologies 4/11/2008 15 Read Head Sensor Technologies Year 1979 Areal Density 10 Mb/in2 (LMR) Sensor Technology Structure Thin-film Inductive 1991 Lead MR Sensor (LMR) 1997 2 Gb/in2 NiFe Free Layer Hard Bias Lead Hard Bias Spacer NiFeX SAL Lead N/A N/A Barkhausen Johnson Anisotropic MR Hard Bias Cu Spacer NiFe Free Layer 2006 Tunnel Valve (PMR) Johnson Lead Spacer Hard Bias Insulator Johnson Bottom Shield Shield CoFe/NiFe Free Layer Spacer Hard Bias Insulator Lead Giant MR Shield 100 Gb/in2 CIP (Current In Plane) Shield Lead Hard Bias (LMR) Major Noise Sources Shield Insulator AP Pinned Co Layer Spin Valve Current Geometry Shield Insulator 100 Mb/in2 MR Effect Tunneling MR MgO Tunnel Barrier AP Pinned CoFeB Layer Shield CPP (Current Perpendicular to the Plane) Johnson Shot Noise Mag Noise Shield Shield 2011 1 Tb/in2 (PMR) CPP GMR High spin-scattering Free Layer Spacer Spacer Hard Bias Hard Bias Insulator Insulator High spin-scattering Pinned Layer © 2008 Hitachi Global Storage Technologies Cu Spacer Shield Giant MR Shield Johnson Mag Noise Spin Torque 4/11/2008 16 Read Head Sensor Challenges Migration to Low RA Sensors Read Head Challenges 500 – Track width – Shield spacing • High Sensitivity (mV/Oe) ∆V = i η (∆R/R) R • Low Noise – Johnson Noise – Shot Noise (TMR) – Mag Noise 2 0.4 Ω - μ m 400 2 1 Ω- μm (RA Product) 2 0.15 Ω - μ m 300 2 0.1 Ω - μ m TMR Current Screen CPP-GMR All Metal CPP- GMR 200 Migration to Low RA Sensors ~TW 2 0.05 Ω - μ m TW 100 • Design Constraints – – – – – Sensor resistance (Ω) • Small Geomerty 50 Ω < R < 500 Ω Temperature Rise Breakdown Voltage Spin Torque Instability Magnetic Self-Field Sensor Resistance R = (RA / TW 2 ) 0 0 10 20 30 40 50 60 70 80 Track Width (nm) (~ Stripe Height) Read Head Requirements Requirement 300 Gbit/in2 500 Gbit/in2 750 Gbit/in2 1000 Gb/in2 2000 Gb/in2 Track Width 60 nm 45 nm 35 nm 27 nm 20 nm Shield Spacing 35nm 32nm 30nm 22nm 20nm SNR 33 dB 32 dB 31 dB 30 dB 30 dB © 2008 Hitachi Global Storage Technologies 4/11/2008 17 AMR, GMR and TMR Physical Mechanisms 1991 AMR (CIP) ΔR/R ~ 2% t ~ 100 nm NiFe e− M Mechanism : Spin orbit scattering. Resistance lower when current flow is parallel to the magnetization M. Limitation : Surface scattering limits film thickness to > 100 nm. GMR (CPP) M2 M1 e− FM1 Cu FM2 2010? ΔR/R ~ 10% Mechanism : Same as CIP GMR. No parasitic resistance problem. Low noise, but lower ΔR/R than TMR. Limitation : Spin torque, and “mag noise” due to thermal fluctuations in M. © 2008 Hitachi Global Storage Technologies GMR (CIP) FM1 Cu FM2 M2 M1 1997 ΔR/R ~ 10-15% e− Mechanism : Spin dependent scattering. With M1||M2, half the electrons (the majority electrons) have low scattering in both films. With M1 anti || M2, all electrons have high scattering in one of the films. It turns out that M1||M2.has lower resistance. Limitation : CIP lead parasitic resistance. TMR (CPP) M2 M1 e− E low scattering high scattering EF majority electrons minority electrons D(E) D(E) 2006 FM1 MgO FM2 ΔR/R >= 100% (room temp) Mechanism : Spin dependent tunneling. FM1 imparts a spin polarization : more min conduction e−. When M1||M2, these min e− have more states to tunnel into. So M1||M2 is the lower resistance state. Limitation : High resistance as sensor size shrinks. 4/11/2008 18 Future Readback Sensor Candidates Extraordinary Magnetoresistance Magnetic Tunnel Transistor Spin Accumulation Sensor Physics: Lorentz force + electrostatics in semiconductor /metal heterostructures Solin et al, JVST B 21, 3002 (2003) Coulomb Blockade Magnetoresistance Physics: Hot electron transport + spin dependent transmission Park et al, JAP 98, 103701 (2005) Spin FET Jedema et al, APL 81, 5162 (2002) Tunneling Anisotropic Magnetoresistance Physics: Single electron transport + spin dependent chemical potential Wunderlich et al, PRL 97, 077201 (2006) © 2008 Hitachi Global Storage Technologies Physics: Spin polarized injection and extraction + Hall et al, Rashba effect APL 83, 2937 (2003) Giddings et al, PRL 94, 127202 (2006)) 4/11/2008 19 Extraordinary Magnetoresistance (EMR) Sensor 2 DEG Current Density × Applied Field Linear Response with ΔR/R ~ CIP GMR External Field 2005 EMR Device Electrons 0.13 Metal Shunt y = 6.2e-006*x + 0.13 ΔV EMR~ 6 mV @ 650 Oe ΔVEMR/ΔH ~ 6 μV/Oe 0.129 2 DEG V2-4 [V] 0.128 0.127 0.126 Applied Current Measured Voltage + 0.125 0.124 -500 2006 Device © 2008 Hitachi Global Storage Technologies -400 -300 -200 -100 0 100 BApplied [Gauss] 200 300 400 500 Noise still a problem : lower SNR than TMR. 4/11/2008 20 Iterative Decoding (LDPC Decoding) Iterative Decoding Issues Parity Check Nodes LDPC Decoder Bit Nodes • Implementation complexity, speed and latency. • Decoding error floors. • Miscorrection detection. • Burst correction. readback samples readback samples PR equalizer PR equalizer bit probabilities SISO Detector Parity Post Proc Viterbi Plus Error Filters SISO detector iteration LDPC decoder RS ECC decoder RS ECC decoder detected data detected data soft decisions (bit probabilities) hard decisions (bits) © 2008 Hitachi Global Storage Technologies 4/11/2008 21 Agenda Overview of Hitachi GST & San Jose Research Center Technology Challenges for Magnetic Recording Future Recording Directions Patterned Media Thermally Assisted Recording © 2008 Hitachi Global Storage Technologies 4/11/2008 22 Patterned Media Conventional PMR Media • Continuous granular recording layer. • Multiple grains per bit. • Boundaries between bits determined by grains. • Thermal stability unit is one grain. © 2008 Hitachi Global Storage Technologies Bit Patterned Media • Highly exchange coupled granular media. • Multiple grains per island, but each island is a single domain particle. • Bit locations determined by lithography. • Thermal stability unit is one island. Discrete Track Media • Conventional PMR media, with patterned tracks. • Multiple grains per bit. • Eliminates track edge noise and increases tolerance to TMR. • Thermal stability unit is still one grain. 4/11/2008 23 Patterned Media Fabrication Process Template Fabrication Media Fabrication Process PMR Media Deposition Template Replication Rotary Stage E-Beam Patterning Nanoimprint Master Template Fabrication Template Replication Pattern Transfer (i.e. etch/mill into recording layer) Planarization One e-beam master template 10,000 replica nanoimprint molds Existing Processes New Processes Lube and Burnish 100,000,000 imprinted disk substrates Inspection © 2008 Hitachi Global Storage Technologies 4/11/2008 24 Thermally Assisted Recording (TAR) • Using new magnetic media, heat is applied for ease of writing data • Heat media to record data but store and read data at normal temperature • Enables use of very difficult to write highenergy media, which is more stable for writing data • May allow areal density in the terabit/square inch range, similar to patterned media GMR laser write coils heat spot © 2008 Hitachi Global Storage Technologies 4/11/2008 25 Thermally Assisted Recording (TAR) Challenges • Development of new small grain high coercivity media with correct thermal properties. • Recording head writer design with optical waveguide and near field source. • Head-disk interface & contamination. • Light coupling efficiency from laser, through waveguide and near field source. • Spot size converter, polarization rotator. • Power dissipation and thermal management in the recording head. • Cost of laser and assembly per slider. • Thermal timing and side writing on neighboring tracks. © 2008 Hitachi Global Storage Technologies 4/11/2008 26 HDD Future Technology Roadmap HDD Future Technology • Conventional PMR technology likely extendable to 1 Tb/in2 or more. • Magnetic storage technology extendable to very high areal densities. 20,000? Areal Density Thermally Assisted Recording (TAR) Possibly combined with PM 5,000? Patterned Media (PM) (DTR & BPM) 1000? Perpendicular Recording 130 Longitudinal Recording • 50 Years • >50 Million increase in areal density Time © 2008 Hitachi Global Storage Technologies 4/11/2008 27 Changing Markets and Usage Requirements New Applications • • • • Portable storage Near line storage Set Top Boxes/PVR Gaming Emerging Technical Requirements • Security Features (bulk encryption) • Reduced power consumption for data centers New Storage Interfaces New Competing Technologies Continued Growth in Capacity Requirements © 2008 Hitachi Global Storage Technologies 4/11/2008 28 Summary The HDD industry is at a technology crossroads. Transition to future technologies will be more difficult than transition from longitudinal to perpendicular recording. Faster rate of technology introduction. • Many new technologies required to reach 1 Tb/in2 in ~2011. Technologies must be introduced while reducing cost (average prices declining about 5% per year). Magnetic recording technology continues to be very extendable, but investing in the R&D and in new technology introduction is challenging. © 2008 Hitachi Global Storage Technologies 4/11/2008 29