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Intermetallic RE<sub>6</sub>T<sub>5</sub>Al<sub>7</sub> Phases (RE = Sc, Y, Ce–Nd, Sm, Gd–Lu; T = Ru, Ir): Diversity in their Magnetic, Magnetocaloric, and Critical Properties

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Citations

52

References

2019

Year

Abstract

Over 20 new compounds of the RE<sub>6</sub>T<sub>5</sub>Al<sub>7</sub> series (RE = Sc, Y, Ce-Nd, Sm, Gd-Lu; T = Ru, Ir; Yb<sub>6</sub>Ir<sub>5</sub>Ga<sub>7</sub> type structure; superstructure of MgZn<sub>2</sub>; fully ordered Nb<sub>6.4</sub>Ir<sub>4</sub>Al<sub>7.6</sub> type) have been synthesized. They crystallize in the hexagonal crystal system with space group <i>P</i>6<sub>3</sub>/<i>mcm</i>. Their lattice parameters are in the ranges of <i>a</i> = 935-963 and <i>c</i> = 851-874 pm for the RE<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> and <i>a</i> = 913-966 and <i>c</i> = 825-865 pm for the RE<sub>6</sub>Ir<sub>5</sub>Al<sub>7</sub> series. Four structures (Ho<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub>, Yb<sub>6</sub>Ru<sub>4.68(1)</sub>Al<sub>7.32(1)</sub>, Sc<sub>6</sub>Ir<sub>5</sub>Al<sub>7</sub>, and Ho<sub>6</sub>Ir<sub>4.53(1)</sub>Al<sub>7.47(1)</sub>) have been refined from single-crystal data, indicating fully ordered structures for Ho<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> and Sc<sub>6</sub>Ir<sub>5</sub>Al<sub>7</sub>; however, T/Al mixing was observed on one crystallographic site for Ho<sub>6</sub>Ir<sub>4.53(1)</sub>Al<sub>7.47(1)</sub> and on two sites for Yb<sub>6</sub>Ru<sub>4.68(1)</sub>Al<sub>7.32(1)</sub>. The Sc-, Y-, and Lu-containing compounds exhibit Pauli paramagnetism in line with a filled d band for Ru and Ir. Ce<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> exhibits mixed-valent behavior, while Yb<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> is solely trivalent. The other compounds exhibit paramagnetism and ferromagnetic phase transitions up to temperatures of <i>T</i><sub>C</sub> = 83.4(1) K for Gd<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub>. In addition to the basic magnetic characterizations and studies of the electrical resistivity and heat capacity, the magnetocaloric properties of Gd<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub>, Tb<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub>, and Dy<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> have been investigated, revealing magnetic entropy changes of -Δ<i>S</i><sub>M</sub><sup>max</sup> = 6.2(1), 7.7(1), and 5.4(1) J kg<sup>-1</sup> K<sup>-1</sup> (0 → 5 T) and relative cooling powers RCP = 242, 207, and 135 J kg<sup>-1</sup>, respectively. For a deeper insight into the second-order magnetic phase transitions, the critical behavior was investigated according to the scaling hypothesis. The critical behavior of Gd<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> is in accordance with the mean-field theory; the critical exponents of Tb<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub> and Dy<sub>6</sub>Ru<sub>5</sub>Al<sub>7</sub>, however, deviate strongly from this universality class. For comparison of the structural and magnetic properties, the thus far unstudied members of the RERuAl series (RE = Sc, Y, Sm, Gd-Lu; MgZn<sub>2</sub> type) have additionally been prepared and characterized.

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