Abstract <p>Thermogravimetric analysis with simultaneous DTA signal recording is performed for lanthanum tris-dipivaloylmethanate, [La(dpm)<sub>3</sub>]<sub>2</sub>. An endothermic effect associated with an irreversible phase transition is revealed in the 455-474&#xa0;K range. The phase transition temperature of 455.2&#xa0;±&#xa0;0.5&#xa0;K is established by differential scanning calorimetry. Crystals of the high-temperature phase are obtained from the gas phase by sublimation transport in an evacuated sealed ampoule under a temperature gradient from 470&#xa0;K to 480&#xa0;K. It is shown by single-crystal XRD that the observed phase transition is caused by a change in the [La(dpm)<sub>3</sub>]<sub>2</sub> molecular structure. The high‑temperature isomer (triclinic, <i>a</i>&#xa0;=&#xa0;11.43&#xa0;Å, <i>b</i>&#xa0;=&#xa0;12.98&#xa0;Å, <i>c</i>&#xa0;=&#xa0;15.14&#xa0;Å, α&#xa0;=&#xa0;101.5°, β&#xa0;=&#xa0;101.0°, γ&#xa0;=&#xa0;113.6°, <i>V</i>&#xa0;=&#xa0;1929&#xa0;Å<sup>3</sup>, <i>Z</i>&#xa0;=&#xa0;1) is also formed by dimeric molecules, but the coordination environment of the lanthanum atom changes from a distorted trigonal monocapped prism (CN&#xa0;=&#xa0;7) to a distorted square antiprism (CN&#xa0;=&#xa0;8), and the number of μ<sub>2</sub>-oxygen atoms increases from 2 to 4.</p>

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Phase Transition in Lanthanum Tris(dipivaloylmethanate) near 455 K: Thermal and Structural Analysis

  • A. S. Sukhikh,
  • D. A. Ulybin,
  • I. V. Korolkov,
  • S. V. Sysoev,
  • P. A. Stabnikov,
  • M. A. Bespyatov

摘要

Abstract

Thermogravimetric analysis with simultaneous DTA signal recording is performed for lanthanum tris-dipivaloylmethanate, [La(dpm)3]2. An endothermic effect associated with an irreversible phase transition is revealed in the 455-474 K range. The phase transition temperature of 455.2 ± 0.5 K is established by differential scanning calorimetry. Crystals of the high-temperature phase are obtained from the gas phase by sublimation transport in an evacuated sealed ampoule under a temperature gradient from 470 K to 480 K. It is shown by single-crystal XRD that the observed phase transition is caused by a change in the [La(dpm)3]2 molecular structure. The high‑temperature isomer (triclinic, a = 11.43 Å, b = 12.98 Å, c = 15.14 Å, α = 101.5°, β = 101.0°, γ = 113.6°, V = 1929 Å3, Z = 1) is also formed by dimeric molecules, but the coordination environment of the lanthanum atom changes from a distorted trigonal monocapped prism (CN = 7) to a distorted square antiprism (CN = 8), and the number of μ2-oxygen atoms increases from 2 to 4.