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X-ray magnetic circular dichroism: Looking at magnets in the right light

Looking at magnets in the right light
Artist's impression of the XMCD experiment. The soft-x-ray light from a plasma source is first circularly polarized by the transmission through a magnetic film. Subsequently, the magnetization in the actual sample can be determined accurately. Credit: Christian Tzschaschel

Magnetic nanostructures have long been part of our everyday life, e.g., in the form of fast and compact data storage devices or highly sensitive sensors. A major contribution to the understanding of many of the relevant magnetic effects and functionalities is made by a special measurement method: X-ray magnetic circular dichroism (XMCD).

This impressive term describes a fundamental effect of the interaction between light and matter: In a ferromagnetic material, there is an imbalance of electrons with a certain , the spin. If one shines circularly polarized light, which also has a defined angular momentum, through a ferromagnet, a clear difference in transmission for a parallel or anti-parallel alignment of the two angular momenta is observable—a so-called dichroism.

This circular dichroism of magnetic origin is particularly pronounced in the soft-X-ray region (200 to 2000 eV energy of the light particles, corresponding to a wavelength of only 6 to 0.6 nm), when considering the element-specific absorption edges of transition metals, such as iron, nickel, or cobalt, as well as rare earths, such as dysprosium or gadolinium.

Looking at magnets in the right light
The averaged transmission through the investigated sample at the Fe L absorption edges (black data points) can be measured precisely and is well described by a simulation (black line). At the two absorption maxima, see insets, significant dichroism for the two different directions of saturation magnetization of the sample is observable. So far, such experiments have only been possible at large-scale facilities. Credit: Forschungsverbund Berlin e.V. (FVB)

These elements are particularly important for the technical application of magnetic effects. The XMCD effect allows for precisely determining the magnetic moment of the respective elements, even in buried layers in a material and without damaging the sample system. If the circularly polarized soft-X-ray radiation comes in very short femto- to picosecond (ps) pulses, even ultrafast magnetization processes can be monitored on the relevant time scale.

Until now, access to the required X-ray radiation has only been possible at scientific large-scale facilities, such as synchrotron-radiation sources or free-electron lasers (FELs), and has thus been strongly limited.

A team of researchers around junior research group leader Daniel Schick at the Max Born Institute (MBI) in Berlin has now succeeded for the first time in realizing XMCD experiments at the absorption L edges of iron at a of around 700 eV in a laser laboratory. A laser-driven plasma source was used to generate the required soft X-ray light, by focusing very short (2 ps) and intense (200 mJ per pulse) optical laser pulses onto a cylinder of tungsten.

The generated plasma thereby emits a lot of light continuously in the relevant spectral range of 200-2000 eV at a pulse duration of smaller than 10 ps. However, due to the stochastic generation process in the plasma, a very important requirement to observe XMCD is not met—the polarization of the soft-X-ray light is not circular, as required, but completely random, similar to that of a .

Looking at magnets in the right light
Magnetic asymmetry behind the polarizer and the examined sample at the Fe L absorption edges. The two colors correspond to measurements with reversed magnetization of the polarizer - the magnetization direction of the sample is immediately evident from the sign of the dichroism observed (blue vs. red curve). The measurements can be reproduced very accurately by simulations (lines). Credit: Forschungsverbund Berlin e.V. (FVB)

Therefore, the researchers used a trick: the X-ray light first passes through a magnetic polarization filter in which the same XMCD effect as described above is active. Due to the polarization-dependent dichroic transmission, an imbalance of light particles with parallel vs. anti-parallel angular momentum relative to the magnetization of the filter can be generated. After passing through the polarization filter, the partially circularly or elliptically polarized soft-X-ray light can be employed for the actual XMCD experiment on a magnetic sample.

The work, published in the journal Optica, demonstrates that laser-based X-ray sources are catching up with large-scale facilities.

"Our concept for generating circularly polarized soft X-rays is not only very flexible but also partly superior to conventional methods in XMCD spectroscopy due to the broadband nature of our light source," says the first author of the study and Ph.D. student at the MBI, Martin Borchert. In particular, the already demonstrated pulse duration of the generated X-ray pulses of only a few picoseconds opens up new possibilities to observe and ultimately understand even very fast magnetization processes, e.g., when triggered by ultrashort light flashes.

More information: Martin Borchert et al, X-ray magnetic circular dichroism spectroscopy at the Fe L edges with a picosecond laser-driven plasma source, Optica (2023). DOI: 10.1364/OPTICA.480221

Journal information: Optica

Citation: X-ray magnetic circular dichroism: Looking at magnets in the right light (2023, April 5) retrieved 3 October 2023 from
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