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Description of scientific projects

1) Spin dynamics in magnetic alloys and multilayers using femtosecond laser high harmonics

The next important step in understanding of spin dynamics in magnetic alloys and multilayers requires examination of optically induced transients with femtosecond time resolution and element-selectivity. Requirements for such measurements were only recently met by strong progress in laser-based extreme ultraviolet light (XUV) sources generating femtosecond pulses with photon energies reaching up to 72 eV. Such high-energy photons are produced when an intense, laser pulse is focused into a collection of gas atoms, generating high-order harmonics of the fundamental light. Tuning the XUV probe beam to a chosen absorption edge, results in a resonant increase of the signal for the corresponding element.
In our recent experiments, we combined element selectivity with femtosecond time resolution to study magnetic response of Ni/Ru/Fe multilayers. By exciting the multilayer with near infrared laser light we observed the evolution of magnetization response in the Ni and Fe layers simultaneously but separately using synchronized XUV probe pulses (see the Figure below this section). Following the excitation, we detected a fluence-dependent magnetization quenching. Unexpectedly, we also observed magnetization enhancement in the Fe layer for parallel alignment of Fe and Ni magnetization. We ascribed the observed response to the optically generated superdiffusive spin currents between the layers (see Rudolf et al., Nature Communication 2012) – a very new physical phenomenon described theoretically only a few months before the experimental observation.




Adam-UltrafastSpin Dynamics


Top: Experimental setup: an ultrashort laser pulses (red) excite the magnetic sample before it is probed by a train of XUV pulses (blue). Inset: The reflected XUV radiation is diffracted by an optical grating fabricated directly on top of the sample and detected by the X-Ray CCD camera. Bottom: Experimentally measured time- and layer-resolved spin dynamics for Ni/Ru/Fe trilayer. The magnetic asymmetry at the Fe 3p absorption edge (52eV) decreases for antiparallel and is anomalously enhanced for the parallel magnetic orientation of Ni and Fe layers.

2) Ultrafast magnetization dynamics in magnetic thin films, complex alloys and multilayers measured using visible light

In order to investigate the time evolution of the average magnetization of a thin film after optical excitation, we employ an all-visible pump-probe setup. The magnetic response is probed at a central wavelength of 400nm (3eV) using the magneto-optical Kerr effect (MOKE) in longitudinal or polar geometry, while the excitation of the electron system is carried out at a central wavelength of 800nm (1.5eV).

A femtosecond laser amplifier system with pulse energies of up to 1mJ, a repetition rate of 1kHz and pulse durations down to 50fs is used as a light source for the experiment. The mirror alignment can be easily switched between polar and longitudinal geometries to address either the out-of-plane or in-plane components of the sample magnetization.

The experiment can study optically-induced dynamics with a temporal resolution below 100fs and is designed to provide important complementary information to our IR- pump XUV-probe experiments. It provides access to femtosecond magnetization dynamics in the valence and conduction bands of 3d transition metals and their alloys, magnetic multilayer systems, as well as novel rare earth–transition metal materials.

Adam-UltrafastSpin Dynamics

Adam-UltrafastSpin Dynamics

Top: Schematics of our all-optical pump-probe experiment in longitudinal configuration for all-optical measurements of ultrafast demagnetization dynamics. Bottom: Typical ultrafast drop of the magneto-optical signal measured at a Ni sample in our MOKE setup after the excitation with a strong laser pulse at t=0.


3) All-optical switching in magnetic superlattices

It has been known for some time that magnetic moment of a certain ferrimagnetic alloys can be completely reversed using ultrafast pulses of circularly polarized light without an external magnetic field [1]. Although this effect has been first observed in relatively complex ferrimagnetic alloys more recent discovery shows that also ferromagnetic superlattices can be switched by light [2]. This extraordinary discovery opens door to their applications in novel magnetic memories and spintronics applications.

In our project we grow ferromagnetic superlattices on silicon and glass substrates for reflection and transmission geometries, respectively and investigate their switching depending on material and laser beam properties. A femtosecond laser oscillator and a quarter wave plate are used as a light source for the experiments (see Figure below). The response of the region swept by laser beam is analyzed using either Kerr or Faraday imaging or magnetic force microscopy. The example of the optically switched magnetic sample (darker lines marked by arrows) is shown in the figure below as inset.

Adam-All-optical-switchinga) Schematics of all-optical switching and domain imaging setup. b) Darker lines on the bright background show demagnetized domain formation due to right (red) and left (blue) polarized light exposure.

[1] Stanciu, C. D., et al. "All-optical magnetic recording with circularly polarized light." Phys. Rev. Lett. 99, 4 (2007).
[2] Lambert, Charles-Henri, et al. "All-optical control of ferromagnetic thin films and nanostructures." Science 345, 6202 (2014).


4) Magnetic resonant scattering of high-order laser harmonics in the extreme ultraviolet spectral range

Ultrashort pulsed light sources in the extreme ultraviolet (XUV) spectral range (20-250eV) provide a unique possibility to study laser-induced spin dynamics in nanometer-sized magnetic domains. Therefore, we set up a resonant magnetic scattering (RMS) experiment using a laser-driven HHG source. Our experimental approach includes a multilayer mirror pair as a monochromator and a CCD camera to detect the scattered photons in transmission geometry. The resulting image is directly related to the domain structure. With the advantage of the high coherence and superior time resolution of the laser-generated high-order harmonics, RMS allows jitter-free pump-probe studies of the dynamics of magnetic domain quenching with femtosecond temporal and nanometer lateral resolution. Additionally, element-selectivity can be also employed in this method to support time-resolved investigations of complex alloys and multilayer systems. 

Adam-Mag-res-scatteringSchematics of the magnetic scattering setup using HHG source (left) and the measured scattering image from a Co/Pt-multilayer (right).

5) Novel sources of pulsed vacuum ultraviolet light

X-Rays and Extreme Ultraviolet Radiation (XUV) play an important role in many areas of today’s research and manufacturing processes. The development of more brilliant sources for this spectral range can lead the path to new levels of manufacturing detail such as smaller integrated circuits, more precise analytics tools in solid-state physics such as spectro-holography or new exciting ways in biological imaging such as phase-contrast microtomography.

In our experiment we aim for the creation of XUV by illuminating micrometer-sized metallic particles with a powerful laser beam. The particles fall from a reservoir through a small tube similar to an hourglass. They have a size of 30µm to 1.5µm and can consist of different metals such as Pb, Sn, Sb, Zn, Al, Cu, or steel. The laser energy excites the electrons in the particles into a higher energy state. Radiation is emitted, when the electrons return to their prior states. The particle gets completely vaporized, thus for continuous operation, new targets must replace the vanished frequently.

The overall goal is to develop a highly brilliant source for XUV- and X-Rays with pulse duration in the femtosecond range. The project is conducted in collaboration with the Moscow Power Engineering Institute (MPEI).

Adam-XUVSchematics of experimental setup for XUV-light generation from metallic microtargets.