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    AlFe<sub>2–<i>x</i></sub>Co<sub><i>x</i></sub>B<sub>2</sub> (<i>x</i> = 0–0.30): <i>T</i><sub>C</sub> Tuning through Co Substitution for a Promising Magnetocaloric Material Realized by Spark Plasma Sintering

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    AlFe<sub>2</sub>B<sub>2</sub> and AlFe<sub>2–<i>x</i></sub>Co<sub><i>x</i></sub>B<sub>2</sub> (<i>x</i> = 0–0.30) were synthesized from the elements in three different ways. The samples were characterized by powder X-ray diffraction, Rietveld refinements, energy-dispersive X-ray spectroscopy, and magnetic measurements. Using Al flux the formation of AlFe<sub>2</sub>B<sub>2</sub> single crystals is preferred. Arc melting enables the substitution of ∼6% Co. This substitution of Fe by Co decreases the Curie temperature <i>T</i><sub>C</sub> from 290 to 240 K. The highest Co substitution up to 15% is achieved by spark plasma sintering (SPS). <i>T</i><sub>C</sub> is reduced to 205 K. In all cases an excess of Al is necessary to avoid the formation of ferromagnetic FeB. Al<sub>13</sub>Fe<sub>4–<i>x</i></sub>Co<sub><i>x</i></sub> is the common byproduct. <i>T</i><sub>C</sub> and the cobalt content are linearly correlated. The transition paramagnetic–ferromagnetic remains sharp for all examples. The magnetic entropy change of the Co-containing samples is comparable to AlFe<sub>2</sub>B<sub>2</sub>. SPS synthesis yields, in short reaction times, a homogeneous and dense material with small amounts of paramagnetic Al<sub>13</sub>Fe<sub>4–x</sub>Co<sub><i>x</i></sub> as an impurity, which can serve as sinter additive. These properties make AlFe<sub>2–<i>x</i></sub>Co<sub><i>x</i></sub>B<sub>2</sub> a promising magnetocaloric material for applications between room temperature and 200 K
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