On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic...

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H. C. Siegmann, C. Stamm, I. Tudosa, Y. Acremann ( Stanford ) On the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory Collaborators: A. Vaterlaus (ETH Zürich) A. Kashuba (Landau Inst. Moscow) ; A. Dobin (Seagate) D. Weller, G. Ju, B.Lu (Seagate Technologies) G. Woltersdorf, B. Heinrich (S.F.U. Vancouver) samples theory magnetic imaging

Transcript of On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic...

Page 1: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

H. C. Siegmann, C. Stamm, I. Tudosa, Y. Acremann ( Stanford )

On the Ultimate Speed of Magnetic Switching

Joachim Stöhr

Stanford Synchrotron Radiation Laboratory

Collaborators:

A. Vaterlaus (ETH Zürich) A. Kashuba (Landau Inst. Moscow) ; A. Dobin (Seagate)

D. Weller, G. Ju, B.Lu (Seagate Technologies)G. Woltersdorf, B. Heinrich (S.F.U. Vancouver) samples

theorymagnetic imaging

Page 2: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

The ultrafasttechnology

gap

want to reliablyswitch smallmagnetic “bits”

The Technology Problem: Smaller and Faster

Page 3: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

186 years of “Oersted switching”….

How can we switch faster ?

Page 4: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Faster than 100 ps….Mechanisms of ultrafast transfer of energy and angular momentum

Optical pulse

Most direct way:Oersted switching

Precessional or ballistic switchingExchange switching (spin injection)

Shockwave

IR or THz pulseElectrons Phonons

Spin

τ ~ 1 ps

τ = ? τ ~ 100 ps

Page 5: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Precessional or ballistic switching:

Discovery

Page 6: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Creation of large, ultrafast magnetic fields

Conventional method

- too slow

Ultrafast pulse – use electron accelerator

C. H. Back et al., Science 285, 864 (1999)

Page 7: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Torques on in-plane magnetization by beam field

Max. torque

Min. torque

Initial magnetization of sample

Fast switching occurs when H M┴

Page 8: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Precessional or ballistic switching: 1999

Patent issued December 21, 2000: R. Allenspach, Ch. Back and H. C. Siegmann

Page 9: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Precessional switching case 1:

Perpendicular anisotropy sample

I. Tudosa, C. Stamm, A.B. Kashuba, F. King, H.C. Siegmann,J. Stöhr, G. Ju, B. Lu, and D. Weller

Nature 428, 831 (2004)

Page 10: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

End of field pulse

M

The simplest case: perpendicular magnetic medium

Page 11: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Pattern of perpendicular anisotropy sample CoCrPt perpendicular recording media (Seagate)

Page 12: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Multiple shot switching of perpendicular sample

Dark areas mean M Light areas mean M

Tudosa et al., Nature 428, 831 (2004)

CoCrPt recording film

Page 13: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Landau-Lifshitz-Gilbert theory Experiment

1 = white

0 = gray

-1 = dark

Intensity profiles thru images

1 shot

2 shots

6 shots 7 shots

curve = M1

curve = (M1)3

curve = (M1)7

curve = (M1)5

curve = (M1)2

curve = (M1)4

curve = (M1)6

Data analysisLandau-Lifshitz-Gilbert theory Experiment

3 shots

5 shots4 shots

Multiplicative probabilities are signature of a random variable.Analysis reveals a memory-less process.

Page 14: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Magnetization fracture under ultrafast field pulse excitation

Non-deterministic region partly due to fractured magnetization

Page 15: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Magnetization fracture under ultrafast field pulse excitation

Macro-spin approximationuniform precession

Magnetization fracturemoment de-phasing

Breakdown of the macro-spin approximation

Tudosa et al., Nature 428, 831 (2004)

Page 16: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Precessional switching case 2:

In-plane anisotropy sample

C. Stamm, I. Tudosa, H.C. Siegmann, J. J. Stöhr, A. Yu. Dobin,G. Woltersdorf, B. Heinrich and A. Vaterlaus

Phys. Rev. Lett. 94, 197603 (2005)

Page 17: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

In-Plane Magnetization: Pattern development

• Magnetic field intensity is large

• Precisely known field size

540o

360o

180o

720o

Rotation angles:

Page 18: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Origin of observed switching pattern

In macrospin approximation, line positions depend on:• angle γ = B τ• in-plane anisotropy Ku• out-of-plane anisotropy K┴• LLG damping parameter α

γ

from FMR data

H increases15 layers of Fe/GaAs(110)

Page 19: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Breakdown of the Macrospin Approximation H increases

With increasing field, deposited energy far exceeds macrospin approximationthis energy is due to increased dissipation or spin wave excitation

Page 20: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Breakdown of the macrospin approximation: why?

Experiments reveal breakdown for short pulse length τ and large B

peak power deposition ~ B2 / τ = α B / τ2

Breakdown appears to be caused by peak power induced fracture of magnetization – non-linear excitations of spin system

Page 21: On the Ultimate Speed of Magnetic Switching · PDF fileOn the Ultimate Speed of Magnetic Switching Joachim Stöhr Stanford Synchrotron Radiation Laboratory ... G. Woltersdorf, B. Heinrich

Conclusions

• The breakdown of the macrospin approximation forfast field pulses limits the reliability of magnetic switching

• Breakdown is believed to arise from energy & angular momentumtransfer within the spin system – excitation of higher spin wave modes

• Details are not well understood….

For more, see: http://www-ssrl.slac.stanford.edu/stohr

and

J. Stöhr and H. C. Siegmann Magnetism: From Fundamentals to Nanoscale Dynamics800+ page textbook ( Springer, to be published in Spring 2006 )