JOURNAL ARTICLE

Giant Negative\nMagnetization in Al<sub>9–<i>x</i></sub>Fe<sub><i>x</i></sub>Mo<sub>3</sub>

Abstract

We present derivatives of the Al<sub>3</sub>Ti-type of\nstructure\nAl<sub>8</sub>FeMo<sub>3</sub> (Al<sub>9–<i>x</i></sub>Fe<sub><i>x</i></sub>Mo<sub>3</sub>) and Al<sub>8</sub>CuMo<sub>3</sub>. Structural features are a molybdenum-square lattice\nand a solid solution of iron (copper) on aluminum sites. By substitution\nof Al with 3d-transition metals outstanding magnetic properties are\nfound. Typical Pauli paramagnetism is observed above a critical temperature <i>T</i><sub>c</sub> ≈ 93 K. Below <i>T</i><sub>c</sub> the series Al<sub>9–<i>x</i></sub>Fe<sub><i>x</i></sub>Mo<sub>3</sub> (0.5 < <i>x</i><sub>Fe</sub> < 1) exhibits the rare coexistence of negative magnetization/diamagnetism\nin zero-field cooling and ferromagnetism in field-cooling mode. For\nAl<sub>8.33</sub>Fe<sub>0.67</sub>Mo<sub>3</sub> the negative magnetization\nis estimated to the order of ∼50% of the diamagnetic response\nof superconducting lead. The contribution of Fe to the magnetization\nis evaluated by <sup>57</sup>Fe Mössbauer spectroscopy in zero\nfield and applied external fields. We show that ferromagnetic fluctuations\noriginate from screened magnetic moments of Fe. The magnetic order\npresumably involves multibands originating from iron and molybdenum\nin the vicinity of the Fermi energy. Further insights into anomalous\nelectron–phonon coupling are gained.

Keywords:
Paramagnetism Ferromagnetism Diamagnetism Superconductivity Pauli exclusion principle Magnetic moment Coupling (piping) Magnetic susceptibility Inductive coupling

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Topics

Quasicrystal Structures and Properties
Physical Sciences →  Materials Science →  Materials Chemistry
Shape Memory Alloy Transformations
Physical Sciences →  Materials Science →  Materials Chemistry
Metallic Glasses and Amorphous Alloys
Physical Sciences →  Engineering →  Mechanical Engineering

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