MOKE magnetometry (Magnetic-Optic Kerr Effect)

When linearly polarised light is reflected from a magnetic film, its polarisation becomes elliptic (Kerr ellipticity) and the polarization principal axis is rotated (Kerr rotation). This rotation is proportional to a component (depending on the geometry of experiment) of the magnetisation of the film. For this reason the MOKE magnetometry is a very popular tool for the characterization of the magnetic properties of materials. With a suitable set-up the sensitivity of the MOKE apparata can be pushed to detect the signal coming from very thin films (ideally down to the atomic plane) making the technique suitable for the study of magnetic structure of thin films, interfaces and nanostructures.

MOKE1 - MBE Cluster

One MOKE apparatus is present on the MBE Cluster growth system. In this set-up is possible to perform MOKE in the longitudinal configuration and to record hysteresis loop measurements in vacuum or on air. In this system (figure) polarized light impinges on the sample located between the poles of the electromagnet. The reflected light passes through the analyzer optical lens, which is set close to extinction. The signal is then detected by a photodiode; the current signal finally passes through a lock in amplifier, giving the Kerr signal of the sample. The optical components are mounted on an optical table.  The sample on the head of the UHV manipulator can be cooled down to 30K (He flow cryostat) and stabilized by feedback at any temperature between 30K and 340K. The azymuthal angle can be varied by 360 degrees (around an axis perperndicular to the surface) enabling the measure of in-plane magnetic anisotropy. The physical dimensions of the Ti-UHV insert chamber limits the electromagnet gap to an effective field of 0.55 T on the sample. Reducing the gap in air allows to measure off-situ samples with H fields up to 0.75 T.


MOKE2 - Surface Lab

Other MOKE systems are available also at the Surface and Nano Science Lab. 3 different types of magnets are installed in the UHV chamber. One magnet is set so as the transversal MOKE measurements can be performed during the growth of epitaxial thin films with e-beam evaporators. The maximum magnetic field is 600 Oe. The 2nd magnet is for the polar MOKE measurement, and the maximum available magnetic field is 3000 Oe. The 3rdmagnet is composed of orthogonally placed 3 non-core coils, which allows to magnetize samples along any direction for MOKE measurements. For all configurations, the sample temperature can be varied from 200K to 650K. The laser beam is first polarized with a polarizer and focused (100um) on the sample with a lens and the reflected beam intensity is measured with a photodiode. For longitudinal and polar MOKE measurements, an analyzer is installed in front of the detector. No modulation technique is applied but the low pass filter in order to remove 100 Hz noise.

Technical specifications

---------MOKE1- MBE Cluster ---------------------------------------------
Laser wavelength / polarization 632.8 nm / linear
Laser source HeNe Thorlabs HNL020L
in UHV sample temperature range 30 - 340 K
Sample azymuthal rotation 360 degree
Maximum H Field 0.55 T in UHV, 0.75 T in air
Minimum H-field step 0.3 mT
Pole face diameter 76 mm
Frequency filter HINDS optical chopper 50KHz
Detector Si, Ge photodiode HINDS DET 200-004
Detector spectral range 350-1100 nm
---------MOKE2- Surface Lab ---------------------------------------------
Laser diode laser 635nm 5mW
Polarizer and Analyzer (if necessary) Glan-Thompson prism
Detector GaAsP photodiode
Spot size approximately 100um
Sample temperature 200 K – 650 K
Max. Magnetic field transversal MOKE 600 Oe, polar MOKE 300 Oe, 3D MOKE 80 Oe

The map of techniques

at MM building at Q2 building at Elettra experimental hall at CNR-IOM cloud at Fermi-T-Rex laboratory Surface & Nano Science Lab, STM/STS PLD XPS & ambient pressure XAS ARPES & Spin ARPES MOKE & Masked deposition system XPS MBE Oxides SPRINT laboratory SEM XRD PVD data repository open data data analysis
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