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Strong and ductile high temperature soft magnets through Widmanstätten precipitates
2023, Han, Liuliu, Maccari, Fernando, Soldatov, Ivan, Peter, Nicolas J., Souza Filho, Isnaldi R., Schäfer, Rudolf, Gutfleisch, Oliver, Li, Zhiming, Raabe, Dierk
Fast growth of sustainable energy production requires massive electrification of transport, industry and households, with electrical motors as key components. These need soft magnets with high saturation magnetization, mechanical strength, and thermal stability to operate efficiently and safely. Reconciling these properties in one material is challenging because thermally-stable microstructures for strength increase conflict with magnetic performance. Here, we present a material concept that combines thermal stability, soft magnetic response, and high mechanical strength. The strong and ductile soft ferromagnet is realized as a multicomponent alloy in which precipitates with a large aspect ratio form a Widmanstätten pattern. The material shows excellent magnetic and mechanical properties at high temperatures while the reference alloy with identical composition devoid of precipitates significantly loses its magnetization and strength at identical temperatures. The work provides a new avenue to develop soft magnets for high-temperature applications, enabling efficient use of sustainable electrical energy under harsh operating conditions.
In situ correlation between metastable phase-transformation mechanism and kinetics in a metallic glass
2021, Orava, Jiri, Balachandran, Shanoob, Han, Xiaoliang, Shuleshova, Olga, Nurouzi, Ebrahim, Soldatov, Ivan, Oswald, Steffen, Gutowski, Olof, Ivashko, Oleh, Dippel, Ann-Christin, v. Zimmermann, Martin, Ivanov, Yurii P., Greer, A. Lindsay, Raabe, Dierk, Herbig, Michael, Kaban, Ivan
A combination of complementary high-energy X-ray diffraction, containerless solidification during electromagnetic levitation and transmission electron microscopy is used to map in situ the phase evolution in a prototype Cu-Zr-Al glass during flash-annealing imposed at a rate ranging from 102 to 103 K s−1 and during cooling from the liquid state. Such a combination of experimental techniques provides hitherto inaccessible insight into the phase-transformation mechanism and its kinetics with high temporal resolution over the entire temperature range of the existence of the supercooled liquid. On flash-annealing, most of the formed phases represent transient (metastable) states – they crystallographically conform to their equilibrium phases but the compositions, revealed by atom probe tomography, are different. It is only the B2 CuZr phase which is represented by its equilibrium composition, and its growth is facilitated by a kinetic mechanism of Al partitioning; Al-rich precipitates of less than 10 nm in a diameter are revealed. In this work, the kinetic and chemical conditions of the high propensity of the glass for the B2 phase formation are formulated, and the multi-technique approach can be applied to map phase transformations in other metallic-glass-forming systems.
Structural and optical properties of (112̅2) InGaN quantum wells compared to (0001) and (112̅0)
2016, Pristovsek, Markus, Han, Yisong, Zhu, Tongtong, Oehler, Fabrice, Tang, Fengzai, Oliver, Rachel A., Humphreys, Colin J., Tytko, Darius, Choi, Pyuck-Pa, Raabe, Dierk, Brunner, Frank, Weyers, Markus
We benchmarked growth, microstructure and photo luminescence (PL) of (112-2) InGaN quantum wells (QWs) against (0001) and (112-0). In incorporation, growth rate and the critical thickness of (112-2) QWs are slightly lower than (0001) QWs, while the In incorporation on (112-0) is reduced by a factor of three. A small step-bunching causes slight fluctuations of the emission wavelength. Transmission electron microscopy as well as atom probe tomography (APT) found very flat interfaces with little In segregation even for 20% In content. APT frequency distribution analysis revealed some deviation from a random InGaN alloy, but not as severe as for (112-0). The slight deviation of (112-2) QWs from an ideal random alloy did not broaden the 300 K PL, the line widths were similar for (112-2) and (0001) while (112-0) QWs were broader. Despite the high structural quality and narrow PL, the integrated PL signal at 300 K was about 4 lower on (112-2) and more than 10 lower on (112-0).