Nanomagnetism
at High Speed
|
For data storage purposes, magnetic vortices can be trapped in
lithographically defined rectangular or circular magnetic patterns.
They are of considerable technological interest because a low stray
magnetic field leads to a magnetic stability and minimizes the cross-talk
between adjacent vortices—two prerequisites for high storage
densities. At low frequencies, magnetic friction (damping) governs
the response as the magnetic moments rotate into the direction of
an applied field. But at gigahertz frequencies and above, precession
is the dominant process. For the microscopic study of such ultrafast
magnetization dynamics, the collaborators developed a novel technique
based on the 70-picosecond-long x-ray pulses of the ALS, which can
be used like light flashes from a strobe to freeze the dynamics
and to acquire a snapshot of the motion of the magnetization.
In their experiment at ALS Beamline 7.3.1.1, a light flash
from a laser activates a gallium arsenide photo switch, which is
integrated into the sample, and launches a 300-picosecond-long electrical
current pulse into a waveguide optimized for the transmission of
short pulses. The current pulse generates a powerful magnetic field
pulse that initiates the dynamics. After a controllable time delay,
an x-ray pulse illuminates the sample, resulting in a photoelectron
image that is then magnified a thousand-fold by the optics of a
photoemission electron microscope (PEEM-2). An electronic (CCD)
camera accumulates the signal from millions of x-ray pulses until
an image of sufficient quality characterizing the current state
of the magnetization of the sample has been obtained.
Laser pulses (red) generate a current pulse, resulting
in a magnetic field that initiates the magnetization dynamics.
X-ray pulses (blue) probe the sample at 100-picosecond
time intervals. The electron image is detected by the photoemission
electron microscope.
About 40 magnetic structures of different sizes and shapes were
patterned by focused ion beam lithography into a 20-nm thick, magnetically
soft cobalt–iron alloy film on a copper waveguide. Four triangular
magnetic domains meeting in the center of a structure give rise
to a vortex where the domain walls intersect, so that the magnetization
curls around the vortex center or core. X-ray magnetic circular
dichroism (XMCD) at transition-metal L edges probes the direction
and size of the element-specific magnetic moments within the domains.
For the cobalt–iron samples, the researchers computed the
images at 100-picosecond intervals over several nanoseconds as the
ratio of two PEEM images acquired at the cobalt L3 and
L2 absorption edges.
Top: Domain structure of magnetic vortices showing the
directions of the magnetization (white arrows), the vortex handedness
(hands), and the out-of-plane core magnetization (green arrows).
Bottom: Simulated trajectories of left- and right-handed
vortices. Red arrows are the vortex acceleration directions.
In this way, they observed two phases of vortex dynamics: an initial
linear acceleration in response to the field pulse, followed by
a gyrotropic (spiraling) motion of the vortex core around the pattern
center. A "hidden" out-of-plane magnetization in the nanometer-scale
vortex core induces a three-dimensional handedness or chirality
in the planar magnetic structure. The result is a precessional motion
of the core parallel to the subnanosecond in-plane field pulse.
The displacement of the core causes an imbalance of the in-plane
magnetization within the structure, creating a magnetostatic field
perpendicular to the displacement that drives the vortex on a spiraling
trajectory. The observed gyrotropic motion corresponds to a subgigahertz
mode seen in micromagnetic simulations and recent magneto-optical
experiments.
Click on the image above to see a time-resolved PEEM movie of
vortex pattern motion over a period of 8 ns after the driving
field pulse. The movie shows the original image (left)
and gradient image (right), with enhanced contrast of
domain walls and vortex core.
Research conducted by S.-B. Choe, A. Scholl, A. Doran, and H.A.
Padmore (ALS); Y. Acremann and J. Stöhr (Stanford Synchrotron
Radiation Laboratory); and A. Bauer (ALS, SSRL, and Freie Universität
Berlin, Germany).
Research funding: U.S. Department of Energy, Office of Basic Energy
Sciences (BES), and Laboratory Directed Research and Development
Program of Berkeley Lab. Operation of the ALS is supported by BES.
Publication about this research: S.-B. Choe, Y. Acremann, A. Scholl,
A. Bauer, A. Doran, J. Stöhr, and H.A. Padmore, "Vortex-driven
magnetization dynamics," Science 304,
420 (2004).
ALSNews
Vol. 246, October 27, 2004 |