Magnetic Data Storage and Nanotechnology Hard Disk Sensors














- Slides: 14
Magnetic Data Storage and Nanotechnology Hard Disk Sensors Switching layer 5 nm Media Magnetic grain 10 nm
Faster than exponential
Technology Changes in Magnetic Data Storage
GMR Reading Head 5 nm Ni. Fe Optimum
Giant Magnetoresistance (GMR) and Spin Filters Parallel Spin Filters Resistance Low B>0 M Opposing Spin Filters Resistance High B=0 M Ni. Fe Cu Co Two filtering mechanisms: • Bulk: Spin-dependent scattering (Scattering length ℓ > ℓ ) • Interface: Spin-dependent reflection (Spin-dependent potential step)
GMR and TMR Reading Heads General principle: • Two ferromagnetic layers separated by a non-magnetic layer. • For B = 0 they have opposite magnetization (1800). • An external B-field forces them parallel (00). • The switch from opposite spin filters to parallel spin filters reduces the resistance. • Obtain maximum sensitivity right at the switching point (90 0). Implementation: • GMR = metallic spacer layer (Giant Magneto-Resistance) • TMR = insulating spacer layer (Tunnel Magneto-Resistance)
GMR vs. TMR (GMR) Current in plane (CIP) (TMR) Current perpendicular to the plane (CPP) TMR has taken over GMR in hard disk reading heads: Larger effect with the current perpendicular to the layers, no shorting by the metal layer.
Magnetic Storage Media Magnetic Force Microscope (MFM) Image Need 102 magnetic particles per bit to average out size and shape variations. Can’t make them smaller (next slide). The ultimate limit: one particle per bit ! 10 nm Co. Pt particles (magnetically isolated by a Cr coating)
Superparamagnetic Limit of the Particle Size: Thermal Switching Energy Barrier E Preferred axis = “easy axis” (c-axis in hcp Co, shape anisotropy) Flip Rate = f exp[- E/k. T] = Attempt frequency Probability per attempt Larmor 109 s-1 frequency ( Lect. 24 ) 40 k. T for several years retention (proportional to the volume)
Magnetic Shape Anisotropy (Dipole Interaction) • Thin film: M parallel to the film • Rod-shaped particle: M parallel to the rod B-field A large external B-field costs energy. Close the field lines internally. (A more quantitative description requires the demagnetizing field Hd. )
Unfavorable when shrinking bit size. More volume for the same area. Favored by the shape anisotropy.
The next Step: Patterned Magnetic Storage Media: One Particle per Bit
“Perfect” Magnetic Particles Can use fewer particles per bit 3 D stacking 2 D stacking Fe. Pt Nanocrystal with Organic Shell