How the Magnet Got Its Stripes
|
 |
Magnetic
stripe domains in 2.53-monolayer (ML) Fe.
|
One issue in magnetic nanostructure research has concerned the
presence of long-range order in a two-dimensional magnetic material
(for example, spins lined up so as to give rise to ferro- or antiferromagnetism).
It has long been established that an isotropic two-dimensional system
of spins (a Heisenberg system) does not carry long-range order at
nonzero temperature and therefore cannot exhibit magnetic properties—as
long as the system is, in fact, isotropic. The magnetic order observed
in today's ultrathin films is usually attributed to the existence
of magnetic anisotropy—a preferred direction for the magnetic moment.
Magnetic anisotropy arises from two sources: the crystal lattice
geometry (magnetocrystalline anisotropy) and the shape of a grain
of the material (shape anisotropy). In an ultrathin film, the magnetocrystalline
anisotropy dominates, and the magnetization is typically perpendicular
to the plane of the film. As the film thickness increases, the competition
between the two anisotropies results in a spin reorientation transition
(SRT) point where the magnetization flips to lie in the plane of
the film.
Because the two magnetic anisotropies cancel each other out at
the SRT, a study of the magnetic phase at the SRT is expected to
provide insight into the secret of two-dimensional magnetic long-range
order. Early experiments showed that the macroscopic magnetization
of a thin film breaks into stripes near the SRT, raising many challenging
questions about the nature of this stripe phase. Answering these
questions requires observation of the magnetic stripes within an
external magnetic field. However, such observations are inhibited
by the difficulty of operating an electron microscope within a magnetic
field. In this experiment, the issue was addressed by using magnetically
coupled layers in which the interlayer coupling served as a virtual
magnetic field.

Left:
Nanostructure "sandwich" of Co, Cu, and Fe/Ni on a Cu(001)
substrate. Right: Element-specific domain imaging reveals the
stripe domains of the Fe/Ni layer within the virtual magnetic
field (JMCo) provided by the Co layer and the interlayer
coupling.
A uniform thickness of ferromagnetic cobalt was separated from
a wedge of ferromagnetic iron/nickel by a nonmagnetic wedge of copper.
The SRT occurs in the Fe/Ni layer, with the magnetic anisotropy
tuned by the Fe film thickness. The interlayer coupling between
the Fe and Co layers serves as an in-plane virtual magnetic field
whose strength is tuned by the Cu spacer layer thickness. The experiment
was performed using PEEM-2 with circularly polarized light from
ALS Beamline 7.3.1.1. Magnetic domain images were obtained by taking
the ratio of L3 and L2 edges, utilizing the effects of x-ray magnetic
circular dichroism. Domain imaging of the Fe/Ni layer revealed how
the stripe domains change as a function of the magnetic anisotropy
(Fe film thickness) and the in-plane magnetic field (Cu film thickness).
Stripe domains as a function of the magnetic
anisotropy (K) and the magnetic field (H). An analysis of this
image reveals a universal dependence of the stripe width on the
magnetic anisotropy and the magnetic field.
The Fe/Ni stripe orientation was aligned with the Co in-plane magnetization,
and the stripe domain width decreased exponentially with increasing
interlayer coupling between the Co and Fe/Ni films. To understand
the experimental observations, the researchers developed a theoretical
model of the ultrathin Fe/Ni film on a two-dimensional square lattice,
relating the stripe domain width to the interlayer coupling and
the perpendicular anisotropy. The results agreed nicely with the
experimental data, taking into account the exchange interaction,
magnetic anisotropy, dipolar interaction, and magnetic Zeeman energy.
Research conducted by Y.Z. Wu and C. Won (University of California,
Berkeley); A. Scholl and A. Doran (ALS); H.W. Zhao (University of
California, Berkeley, and Institute of Physics, Chinese Academy
of Science); X.F. Jin (Fudan University, China); and Z. Q. Qiu (University
of California, Berkeley, and Berkeley Lab).
Research funding: National Science Foundation; U.S. Department
of Energy, Office of Basic Energy Sciences (BES); Chinese National
Science Foundation; Chinese Ministry of Science and Technology;
and Chinese Academy of Science. Operation of the ALS is supported
by BES.
Publication about this research: Y.Z. Wu, C. Won, A. Scholl, A.
Doran, H.W. Zhao, X.F. Jin, and Z.Q. Qiu, "Magnetic stripe
domains in coupled magnetic sandwiches," Phys. Rev. Lett.
93, 117205 (2004).
ALSNews
Vol. 248, December 22, 2004
|