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The role of Fe and Cu additions on the structural, thermal and magnetic properties of amorphous Al-Ce-Fe-Cu alloys

Authors :
Luka Kelhar
Jean-Marie Dubois
Primož Koželj
Janez Zavašnik
Marjeta Maček-Kržmanc
Sašo Šturm
Spomenka Kobe
Jana Ferčič
Source :
Journal of Non-Crystalline Solids. 483:70-78
Publication Year :
2018
Publisher :
Elsevier BV, 2018.

Abstract

Iron and copper are immiscible elements, but can be combined in the presence of a third element such as aluminium or cerium. We varied the additions of immiscible Fe and Cu (ratio y) in the stoichiometric Al20.5Ce41.5(FeyCu1 − y)38 alloys in order to trace their impact on the structure, microstructure, thermal properties and magnetism. By powder X-ray diffraction (PXRD), we found that Fe-rich alloys (0.87 ≤ y ≤ 1) do not completely hinder crystallisation and yield nanocrystalline precipitates. Cu-rich alloys completely vitrify for 0 ≤ y ≤ 0.74 and exhibit a characteristic broad hump in PXRD patterns. DSC shows that Cu-rich alloys exhibit a noticeably lower crystallisation temperature Tx of about 510 K, liquidus temperature Tl at approximately 900 K and a more pronounced drop Δ of the heat flux at the glass transition temperature Tg. These criteria indicate that Cu-rich alloys are better glass formers. Transmission electron microscopy (TEM) shows that the specimens with y = 0 and y = 0.34 are composed of an amorphous matrix with minor impurities of CeO2 nanocrystals, which can only be observed via transmission electron microscopy. However, these nanocrystals do not interfere with the formation of the glassy phase and are therefore inert. Magnetic measurements show that Fe-rich alloys possess higher magnetisation at maximum field (Mmax H), peaking at 3.3 and 3 emu/g for y = 1 and y = 0.87, respectively. From ferromagnetism in the latter two alloys, the behaviour turns to paramagnetism for 0 ≤ y ≤ 0.74. Cryogenic measurements on SQUID show that the sample with y = 0 displays two different temperature regions at 2–50 K and 100–300 K. The first one exhibits nearly pure paramagnetic behaviour with Θ = − 0.7, while the second one shows a highly negative Weiss constant of Θ = − 80.6.

Details

ISSN :
00223093
Volume :
483
Database :
OpenAIRE
Journal :
Journal of Non-Crystalline Solids
Accession number :
edsair.doi...........48a4e16f43af4d2d28953c107cf4d796
Full Text :
https://doi.org/10.1016/j.jnoncrysol.2018.01.003