<p>In the present study, the new ternary rare earth intermetallic compound PrNi<sub>6</sub>Si<sub>6</sub> has been investigated. This work completes the study of the RNi<sub>6</sub>Si<sub>6</sub> series (R = rare earth). While the RNi<sub>6</sub>Si<sub>6</sub> compounds for R = La and Ce adopt the CeNi<sub>6</sub>Si<sub>6</sub>-type (<i>tP</i>52, <i>P</i>4/<i>nbm</i>, No. 125), surprisingly PrNi<sub>6</sub>Si<sub>6</sub> crystallizes in the YNi<sub>6</sub>Si<sub>6</sub> prototype (<i>tP</i>52, <i>P − </i>4<i>b</i>2, No. 117) as do all the heavier lanthanides (but Lu). The YNi<sub>6</sub>Si<sub>6</sub>-type and its homolog CeNi<sub>6</sub>Si<sub>6</sub> are two tetragonal ordered derivative of the cubic NaZn<sub>13</sub>-type structure. Lattice parameters for PrNi<sub>6</sub>Si<sub>6</sub> are <i>a</i> = 7.7846(1) Å, <i>c</i> = 11.2144(1) Å, with a unit cell volume, <i>V</i><sub>obs</sub> = 679.585(5)&#xa0;Å<sup>3</sup>. The temperature dependence of the inverse magnetic susceptibility <i>χ</i><sup><i>−1</i></sup>(T) follows the Curie–Weiss law, with calculated values of the effective magnetic moment (<i>µ</i><sub>eff</sub>) and Weiss temperature (Θ<sub>pm</sub>) of 3.55 <i>μ</i><sub><i>B</i></sub> and − 4.5&#xa0;K, respectively. While the observed <i>µ</i><sub>eff</sub> is very close to the theoretical value of 3.58 <i>µ</i><sub><i>B</i></sub> for the free Pr<sup>3+</sup> ions, a negative value of the Weiss temperature suggests antiferromagnetic interactions in PrNi<sub>6</sub>Si<sub>6</sub>. Magnetization measurements confirm that PrNi₆Si₆ orders antiferromagnetically (AFM) below a Néel temperature (<i>T</i><sub>N</sub>) of 9&#xa0;K. The Ni atoms contribute negligibly to the magnetic properties of this phase. The specific heat of PrNi₆Si₆ is approximately 0.42&#xa0;J&#xa0;K <sup> − 1</sup> &#xa0;g<sup> − 1</sup>. Measurements of electric and thermal transport reveal that PrNi₆Si₆ exhibits metallic behavior across a wide temperature range of 2–900&#xa0;K, accompanied by a relatively low thermal conductivity of around 6 W&#xa0;K<sup> − 1</sup>&#xa0;m<sup> − 1</sup> at room temperature. Such properties, together with its high-temperature refractory behavior, make PrNi₆Si₆ worthy of consideration in technological applications where fairly good electrical conductivity should be accompanied by a limited thermal conductivity.</p> Graphical abstract <p></p>

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The new PrNi6Si6 intermetallic: from crystal structure to thermal and electrical transport properties across a wide temperature range (2–900 K)

  • S. Singh,
  • A. Provino,
  • I. Pallecchi,
  • F. Caglieris,
  • M. Mödlinger,
  • P. Mele,
  • G. Latronico,
  • T. Takeuchi,
  • P. Manfrinetti

摘要

In the present study, the new ternary rare earth intermetallic compound PrNi6Si6 has been investigated. This work completes the study of the RNi6Si6 series (R = rare earth). While the RNi6Si6 compounds for R = La and Ce adopt the CeNi6Si6-type (tP52, P4/nbm, No. 125), surprisingly PrNi6Si6 crystallizes in the YNi6Si6 prototype (tP52, P − 4b2, No. 117) as do all the heavier lanthanides (but Lu). The YNi6Si6-type and its homolog CeNi6Si6 are two tetragonal ordered derivative of the cubic NaZn13-type structure. Lattice parameters for PrNi6Si6 are a = 7.7846(1) Å, c = 11.2144(1) Å, with a unit cell volume, Vobs = 679.585(5) Å3. The temperature dependence of the inverse magnetic susceptibility χ−1(T) follows the Curie–Weiss law, with calculated values of the effective magnetic moment (µeff) and Weiss temperature (Θpm) of 3.55 μB and − 4.5 K, respectively. While the observed µeff is very close to the theoretical value of 3.58 µB for the free Pr3+ ions, a negative value of the Weiss temperature suggests antiferromagnetic interactions in PrNi6Si6. Magnetization measurements confirm that PrNi₆Si₆ orders antiferromagnetically (AFM) below a Néel temperature (TN) of 9 K. The Ni atoms contribute negligibly to the magnetic properties of this phase. The specific heat of PrNi₆Si₆ is approximately 0.42 J K  − 1  g − 1. Measurements of electric and thermal transport reveal that PrNi₆Si₆ exhibits metallic behavior across a wide temperature range of 2–900 K, accompanied by a relatively low thermal conductivity of around 6 W K − 1 m − 1 at room temperature. Such properties, together with its high-temperature refractory behavior, make PrNi₆Si₆ worthy of consideration in technological applications where fairly good electrical conductivity should be accompanied by a limited thermal conductivity.

Graphical abstract