The magneto-optical Kerr effect (MOKE) is
usually the most suitable methods to characterize
magnetic properties of ultrathin films since
the rotation angle of the electric-field
vector of linearly polarized lights is nearly
proportional to the magnetization of the
films. Although we are planning to use x-ray
magnetic circular dichroism (XMCD) in UVSOR,
in-laboratory experiments is also important
for several reasons. First, detailed and
time-consuming characterization is required
especially for the preparation of new magnetic
materials. Since the beamtime in UVSOR is
limited, some in-laboratory equipment is
essential. Second, the measurements in the
applied magnetic field is easier in MOKE
since MOKE detects polarization of the reflected
lights while XMCD scales emitted electrons.
We have just constructed a new ultrahigh
vacuum (UHV, <1×10-8 Pa) system in which in situ MOKE can be
measured (Figs. 1-4). The system contains a standard UHV pumping
unit, a surface cleaning system of sputtering
and annealing of substrates, and a molecular
beam epitaxy (MBE) system. The substrate
can be cooled down to 90-100 K using liquid
nitrogen and to 25-40 K using liquid He.
A magnetic field can be applied to samples
in UHV with a simple electromagnet up to
3000 Gauss (Fig. 4). The magnetic field is not so large but
is usually sufficient for ultrathin films
of 3d elements. Both the polar MOKE geometry
for perpendicular magnetization and the longitudinal
MOKE for in-plane magnetization are available
(Fig. 5). |
|
|
Figure 1: Schematic view of the UHV MOKE chamber. |
Figure 2: Front view of the UHV MOKE chamber. The
magnet part was now replaced as
in Fig.
4. |
Figure 3: Rear-side view of the UHV MOKE chamber. |
| |
Figure 4: UHV compatible electromagnet (ICF253) made of Au-coated pure Fe. |
Figure 5: Typical MOKE geometries.
Typical MOKE data are shown in Fig. 6. The samples were in-plane magnetized Co
(2 and 5 monolayer thickness)
films on Cu(001)
before and after NO (nitric oxide)
adsorption.
The signal-to-noise ratio is
already sufficient
to investigate these types of
magnetic films. |
|
Figure 6: Longitudinal MOKE data of 2 and 5 ML epitaxial
Co films on Cu(001) before and after NO adsorption
at 100 K. Changes in the Kerr intensity and
the coercivity can be found. |
Using the UHV MOKE system, we will investigate
magnetic properties of ultrathin metal
films,
nanowires and nanodots, especially
control
of magnetism using surface chemical
techniques
such as gas deposition.
|