Title: Magnetism and X-Rays:
1Magnetism and X-Rays Past, Present, and A
Vision of the Future
X-rays have come a long way magnetic
imaging, nanoscale, ultrafast
Joachim Stöhr Stanford Synchrotron Radiation
Laboratory Stanford University
Static image
Femtosecond single shot image
Pump-probe 100 picoseconds dynamics
1993
2003
200X
1895
http//www-ssrl.slac.stanford.edu/stohr/index.htm
2Collaborators
SSRL Stanford H. C. Siegmann H. Ohldag Y.
Acremann J. Lüning W. Schlotter S. Andrews J. P.
Strachan V. Chembrolu
Berlin - BESSY S. Eisebitt M. Lörgen O.
Hellwig W. Eberhardt
Berkeley - ALS A. Scholl S. B. Choe A. Bauer
(FU Berlin)
3Magnetic Structure Neutron Scattering
Press release by the Royal Swedish Academy of
Sciences, Nobel Prize in Physics B. N.
Brockhouse and C. G. Shull 1994 Neutrons are
small magnets (that) can be used to study the
relative orientations of the small atomic
magnets. .. the X-ray method has been powerless
and in this field of application neutron
diffraction has since assumed an entirely
dominant position. It is hard to imagine modern
research into magnetism without this aid."
Antiferromagnet NiO
4The New Paradigm Smaller and Faster
Examples Magnetic Devices in Computers
Present Size gt 100 nm, Speed gt 1 nsec Future
Size lt 100 nm, Speed lt 1 nsec
Ultrafast Nanoscale Dynamics
5 What does it take to explore
advanced magnetic materials and phenomena ?
Need techniques that can see the invisible
spatial
resolution lt 300 nm study thin films and
interfaces large cross section for
signal look below the surface
depth sensitivity distinguish
components elemental
(chemical) specificity resolve dynamic motions
time resolution lt 1
nanosecond
X-rays can do all
that ! - so today, one may say It is hard to
imagine modern research into magnetism without
the aid of x-rays!
6Capabilities of X-Rays
Experimental X-Ray Methods
7Experimental X-Ray Absorption Techniques
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9Magnetic Information through Polarization
Dichroism
a few hundred eV
a few eV
10Magnetic Spectroscopy and Microscopy
x-ray "spin"
Soft X-Rays are best for magnetism!
11Fe metal L edge
Kortright and Kim, Phys. Rev. B 62, 12216 (2000)
12Tunable x- rays offer variable interaction cross
sections
electrons
optical light
Photoemission
neutrons
13 Focusing of x-rays offers nanoscale
resolution
14- Experimental Results 1
- The Puzzle of Exchange Bias
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16The Problem Exchange Bias
M
M
H
H
M of blue layer is pinned or exchange
biased
17Example The Spin Valve Sensor
FM1
Cu
FM2
AFM
Giant magnetoresistance effect
18X-Rays-in / Electrons-out - A way to study
Interfaces
FM Co tune to Co edge circular
polarization AFM NiO tune to Ni edge
linear polarization FM Ni(O) tune to Ni edge
circular polarization
19Spectro-Microscopy of Ferromagnets on
Antiferromagnets
Tune to Co edge use circular polarization
ferromagnetic domains
Tune to Ni edge use linear polarization
antiferromagnetic domains
H. Ohldag et al., PRL 86, 2878 (2001).
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21X-Ray Picture of Exchange Bias
Co/IrMn
Co/NiO
Co
NiO
Element specific FM loops
AFM "loop" rotation
Imaging
- The interface is not sharp
- Parallel coupling
- ? AFM axis is rotated at interface
- Free spins 96 of ML - coercivity
- Pinned Spins 4 of ML - bias
- AFM spring is formed
- anchored in bulk
22- Experimental Results 2
- Time resolved imaging of magnetic structures
23x-ray pulse
electron storage ring
24Imaging of Motion of Nanoscale Domains (100 ps)
real image
differential image
25Two pattern with same static structure, but ..
Field response
Field response
Opposite rotation is caused by direction of
vortex core magnetization, i.e. chirality
26- Experimental Results 3
- Beyond 186 years of Oersted switching.
- Magnetic switching by spin currents
27A new way of magnetic switching spin injection
spin current acts like an Exchange field
electric current creates magnetic field
Oersted field
Weak, long range
Strong, short range
28Switching of magnetic memory cells (MRAM)
cell to be switched
better switching by current in wire
switching by Oersted field around wire
current
current
29A new way of magnetic switching spin injection
current becomes spin-polarized
30Samples for spin-injection studies e-beam
lithography
prepared by Jordan Katine, Hitachi Global Storage
100nm
Au 100 Å Cu 1600 Å Co.86Fe.14 40 Å Cu 35
Å Co.86Fe.14 20 Å Ru 8 Å Co.86Fe.14 18 Å PtMn
175 Å Ta 25 Å Cu 200 Å Ta 50 Å
Oersted field
to be switched
polarizes spins
Challenge see thin 4 nm magnetic layer buried
in 250nm of metals!
current
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32STXM image of spin injection structure
100 x 300 nm
x
y
leads for ns current pulses
Detector
33Images before and after spin injection pulse
magnetization has complicated C
state both electrical current and spin current
contribute
34 A Vision of the Future..
Ultrafast pictures -
single shot images with x-ray lasers (XFEL)
35 not enough intensity cannot do
microscopy
36Coming to Stanford in 2008 The first x-ray
laser - LINAC COHERENT LIGHT SOURCE (LCLS)
0 Km
2 Km
3 Km
37A new way to take fast images no lenses !
coherence length smaller than illuminated
area larger than domains
coherence length larger than illuminated area
Can the reciprocal space pattern be inverted ?
38Towards single shot imaging
39True images! - soft x-ray spectro-holography
coherent x-ray beam
Eisebitt, Lüning, Schlotter, Lörgen, Hellwig,
Eberhardt and Stöhr, Nature 432, 885 (2004)
40Is it real?
FT Hologram
STXM
W. F. Schlotter Y. Acremann
Reference hole ? 100 nm
Resolution 30 - 40 nm
41Conclusions
- X-rays have become an important probe of magnetic
materials and phenomena - X-rays offer elemental, chemical and magnetic
specificity with nanoscale spatial resolution - Transmission experiments probe bulk, electron
yield experiments probe surfaces and interfaces - X-rays allow time-dependent studies, paving the
way for picosecond nanoscale technology - Future x-ray sources, new techniques and
instrumentation will allow the complete
exploration of magnetic phenomena in space and
time
For more, see http//www-ssrl.slac.stanford.edu/
stohr
and new textbook (820 pages)
J. Stöhr and H. C. Siegmann Magnetism From
Fundamentals to Nanoscale Dynamics Springer
Verlag, February/March 2006