Ultrafast Manipulation of the Magnetization J Sthr Sara
- Slides: 24
Ultrafast Manipulation of the Magnetization J. Stöhr Sara Gamble and H. C. Siegmann, SLAC, Stanford A. Kashuba Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
Drivers of Modern Magnetism Research: Smaller and Faster The ultrafast technology gap
“for the discovery of giant magnetoresistance” “pinned” “ 0” “ 1” GMR “reads” the magnetization state
from “reading” to “writing” information ? “ 0” “ 1” The big questions: • What are possible switching methods? • What are the physical processes (and intermediate states)? • What limits the speed of switching?
Conceptual methods of magnetization switching Optical pulse Lattice shock t ~ 1 ps electrons move in femtoseconds Electrons Phonons atoms move in picoseconds exchange or spin-orbit ? t ~ 100 ps Spin field pulses or spin currents into magnetic element
Creation of large, ultrafast magnetic fields d o th e m l a n o i t w n o e l v s n o Co - to Use field pulse created by a moving electron bunch
Origin of the fast switching idea… What is the pattern written by a lightning bolt in magnetic rock? 100 k. A in a flash of a few microseconds Magnetization follows the field lines
The world’s biggest lightning bolt Stanford Linear Accelerator Center - SLAC 3 km, 30 Ge. V
Magnetic writing with SLAC Linac beam thin Co film on Si wafer premagnetized 5 ps 1 n. C or 1010 electrons C. H. Back et al. , Science 285, 864 (1999)
In-Plane Magnetization: Pattern development • Magnetic field intensity is large • Precisely known field size no circles around beam ! very different from lightning pattern 540 o Rotation angles: 720 o 180 o 360 o
The pattern written by a picosecond beam field M initial magnetization direction of sample beam damage Max. torque T=Mx. H Min. torque = 0 Fast switching occurs when H ┴ M
Ballistic Switching – From nano to picoseconds Patent issued December 21, 2000: R. Allenspach, Ch. Back and H. C. Siegmann end of field pulse M Relaxation into “down” direction governed by slow spin-lattice relaxation (100 ps) - but process is deterministic ! Precise timing for a=180 o reduces time
Toward femtosecond switching Experiments with sub-ps bunches • reduce bunch length from FWHM t = 5 ps → 140 fs • keep beam energy and charge fixed (~1010 electrons or 1 n. C) • fields B ~ charge / t and E = c B are increased by factor of 35 • our fields have unprecedented strength in materials science: B-field: 60 Tesla E-field: 20 GV/m or 2 V / Angstrom
How does a relativistic e-beam interact with a material ? note E and B fields are defined within and outside e-bunch
Magnetic pattern is severely distorted for short bunch 10 nm Co 70 Fe 30 on Mg. O (110) 140 fs 15 layers Fe on Ga. As (110) 5 ps damaged area
Magnetic pattern is severely distorted --- does not follow circular B-field symmetry Calculation of pattern with Landau-Lifshitz-Gilbert theory known magnetic properties of film, known length, strength, radial dependence of fields B-field only B-field and E-field
Consider effect of giant E-field of beam magnetocrystalline anisotropy caused by anisotropic atomic positions “bonding fields” distort valence charge – static effect Beam field E ~ 1010 V / m = 1 V / Å comparable to “bonding fields” leads to ultrafast distortion of valence charge - all electronic dynamic effect all new “magnetoelectronic anisotropy” – ultrafast !
Magneto-electronic anisotropy is strong ~ E 2 352 or about 1000 times stronger than with previous 5 ps pulses B-field torque E-field torque
Practical Realization of E-field switching • Giant accelerator is impractical • Want to produce pure E-field effect – no B-field effect • Field pulse needs to be fast How about photons ? We know effect is ~E 2 Linear B-field effect cancels over a full cycle
SLAC e-beam pulse corresponds to THz half-cycle pulse 100 fs 10 THz red: SLAC pulse black: THz half cycle pulse true “EM wave”
• Need strong THz radiation - not readily available • Presently only produced by accelerators • Laser generated THz about 100 times weaker at present Can sample handle intense THz pulse ? Heating of sample would be problem….
Compare beam impact region for different pulse lengths same sample: 10 nm Co 70 Fe 30 on Mg. O (110) Magnetic image Topological image by means of SEMPA microscopy Pulse length: 4 ps beam damage Pulse length: 140 fs 35 times shorter pulse & stronger fields cause no heating, no damage !
If there is an E-field - why is there no heating? strong E field should cause current flow - severe Joule heating Potential of a regular linear lattice Co bandwidth DV ~ 3 e. V a Potential along E field direction E ~ 1010 V/m a = 0. 25 nm DV = e E a ~ 2. 5 e. V Offset of “bands” ~ bandwidth potential gradient leads to breakup of conduction path no current flow due to field – no heating
Summary material behave very strange in extreme fields ! • Unusual E and B field effects • No apparent heating or damage by beam • Extreme THz science just starting….
- Ultrafast demagnetization
- Ultrafast magnetism
- Ultrafast
- Ct magnetization curve test
- Magnetization formula
- Magnetic permeability of materials
- Curl of magnetization
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