Synthesis, Physical, and Magnetocaloric Properties of MgZn2‑Type Gd2Al3Rh

Gd2Al3Rh was synthesized from the elements using arc-melting techniques, along with subsequent annealing. The title compound adopts the hexagonal MgZn2 type structure (space group P63/mmc, hP12, Wyckoff sequence hfa) with the Gd atoms found on the Mg positions (4f), the Rh (2a) and Al (6h) atoms occ...

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Veröffentlicht in:Inorganic chemistry 2024-07, Vol.63 (30), p.14086-14092
Hauptverfasser: Eustermann, Fabian, Stegemann, Frank, Janka, Oliver
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Stegemann, Frank
Janka, Oliver
description Gd2Al3Rh was synthesized from the elements using arc-melting techniques, along with subsequent annealing. The title compound adopts the hexagonal MgZn2 type structure (space group P63/mmc, hP12, Wyckoff sequence hfa) with the Gd atoms found on the Mg positions (4f), the Rh (2a) and Al (6h) atoms occupying the two Zn sites of the prototype. In addition, mixing of Rh and Al on both crystallographic positions is observed. The magnetic susceptibility and magnetization experiments were conducted indicating ferromagnetic ordering below the Curie temperature of T C = 51.3(1) K and very high magnetization of 6.96(1) μB at 3 K and 70 kOe. In addition, heat capacity and electrical resistivity measurements were conducted. The magnetocaloric properties of ferromagnetic Gd2Al3Rh have been determined by means of magnetization measurements. For a field change of ΔH = 0 → 50 kOe the magnetic entropy change equals ΔS M max = −4.8 J kg–1 K–1, leading to a relative cooling power of RCP = 283 J kg–1 for the same field change. The adiabatic temperature change was estimated to be ΔT ad max = 2.1 K using the heat capacity data.
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The title compound adopts the hexagonal MgZn2 type structure (space group P63/mmc, hP12, Wyckoff sequence hfa) with the Gd atoms found on the Mg positions (4f), the Rh (2a) and Al (6h) atoms occupying the two Zn sites of the prototype. In addition, mixing of Rh and Al on both crystallographic positions is observed. The magnetic susceptibility and magnetization experiments were conducted indicating ferromagnetic ordering below the Curie temperature of T C = 51.3(1) K and very high magnetization of 6.96(1) μB at 3 K and 70 kOe. In addition, heat capacity and electrical resistivity measurements were conducted. The magnetocaloric properties of ferromagnetic Gd2Al3Rh have been determined by means of magnetization measurements. For a field change of ΔH = 0 → 50 kOe the magnetic entropy change equals ΔS M max = −4.8 J kg–1 K–1, leading to a relative cooling power of RCP = 283 J kg–1 for the same field change. 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For a field change of ΔH = 0 → 50 kOe the magnetic entropy change equals ΔS M max = −4.8 J kg–1 K–1, leading to a relative cooling power of RCP = 283 J kg–1 for the same field change. 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The magnetocaloric properties of ferromagnetic Gd2Al3Rh have been determined by means of magnetization measurements. For a field change of ΔH = 0 → 50 kOe the magnetic entropy change equals ΔS M max = −4.8 J kg–1 K–1, leading to a relative cooling power of RCP = 283 J kg–1 for the same field change. The adiabatic temperature change was estimated to be ΔT ad max = 2.1 K using the heat capacity data.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.inorgchem.4c01887</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-9480-3888</orcidid></addata></record>
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