In-house laboratory

Our in-house laboratory enables us to do synthesis and characterization of magnetic samples.

Synthesis of magnetic nanoparticles

We synthesize magnetic nanoparticles with different shapes, sizes, and compositions for fundamental studies and applications like hyperthermia, catalysis, and energy conversion. Our typical particles are made of Fe, Co, and Ni, and alloys or oxides thereof. Our synthesis methodologies include wet chemistry for the preparation of suspended nanoparticles and incipient wetness impregnation for the preparation of supported nanoparticles (see examples below). We also make composites, e.g. nanoparticles fixated in polymers, for applications such as high-frequency power electronics.

Hematite (α-Fe2O3) nanoparticles in aqueous solution without (left) and with (right) sodium chloride salt [1].
Maghemite (γ-Fe2O3) nanoflowers synthesized by a polyol method and deposited on boron nitride support (left). STEM image of a nanoflower (center). Tomographic reconstruction of the nanoflower showed in the center (right).

Single crystals

Our in-house x-ray Laue diffraction setup allows us to orient single-crystal samples in preparation for x-ray and neutron diffraction experiments at international large-scale facilities. 
Left: Single crystal back-reflection Laue method. Center: Laue diffraction setup for alignment of single crystalline samples. Right: Laue image of a silicon wafer.
If required the aligned crystals can be cut using a dedicated diamond saw. In order to cut single crystal samples in the desired shapes, e.g. to facilitate experiments with electrical field and pressure, we use a wire saw. Using either a tungsten or diamond-dotted wire, the saw is able to produce very fine cuts, without sacrificing much crystal mass, and to a very high precision. This saw is often used in conjunction with the Laue camera, where one can easily remount aligned samples from the camera in the saw, and produce cuts along the desired crystallographic axes.

Magnetometry

Our magnetometry activities focus on characterizing and testing the magnetic samples with static fields up to 3.4 T, high-frequency fields up to 1 MHz and 130 mT, temperatures from 80 K to 1273 K, and controlled gas environment.
The laboratory features commercial instrumentation together with specialized equipment developed in-house, such as an in-situ vibrating sample magnetometer holder, which can characterize the magnetic properties of magnetic samples during a chemical reaction [2]. Recently, the lab has also developed an AC magnetometer to retrieve hysteresis curves at high frequencies (0.1-1 MHz), enabling better characterization for materials used for e.g. cancer treatment and catalytic process heating.
The lab has also recently developed new measurements protocols for AC field calorimetry [3]. AC calorimetry is a method that estimates the heating power from the increase of temperature when applying an AC magnetic field. This is the primary method used today for characterizing the heating power of magnetic nanoparticles.

Vibrating sample magnetometer retrofitted with in-situ sample holder for magnetometry studies in gas controlled atmospheres both reducing and oxidizing. [2]

57Fe Mössbauer spectroscopy

Mössbauer spectroscopy measures the absorption of nuclear gamma rays from a radioactive source (here 57Co/57Fe). The energy is doppler shifted slightly by moving the source with mm/s relative to the sample. The method is highly sensitive to the chemical environment and magnetic order of the sample due to the hyperfine interaction.
We are able to perform spectroscopy at room temperature down to cryogenic temperatures of 20 K, but equipment is being installed that will enable us to achieve a temperature of 4 K in applied fields of 5 T. 
Left: Principle for doing Mössbauer spectroscopy. Right: Top view of cryostat for doing Mössbauer spectroscopy at low temperatures (4-300 K) and high fields (5 T).

References:

[1] E. Brok et al.Crystals (2017): https://doi.org/10.3390/cryst7080248
[2] M. R. Almind et al., Rev. Sci. Instrum (2023) : 
https://doi.org/10.1063/5.0113493
[3] L. G. Hanson et al., IEEE Magnetics Letters (2023): https://doi.org/10.1109/LMAG.2023.3279778


 

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