Na<sub>2/7</sub>Gd<sub>4/7</sub>MoO<sub>4</sub>: a Modulated Scheelite-Type Structure and Conductivity Properties

Abstract

Scheelite-type compounds with the general formula (A1,A2)<sub><i>n</i></sub>[(B1,B2)­O<sub>4</sub>]<sub><i>m</i></sub> (<sup>2</sup>/<sub>3</sub> ≤ <i>n</i>/<i>m</i> ≤ <sup>3</sup>/<sub>2</sub>) are the subject of large interest owing to their stability, relatively simple preparation, and optical properties. The creation of cation vacancies (□) in the scheelite-type framework and the ordering of A cations and vacancies can be a new factor in controlling the scheelite-type structure and properties. For a long time, cation-deficient Nd<sup>3+</sup>:M<sub>2/7</sub>Gd<sub>4/7</sub>□<sub>1/7</sub>MoO<sub>4</sub> (M = Li, Na) compounds were considered as potential lasers with diode pumping. They have a defect scheelite-type 3D structure (space group <i>I</i>4<sub>1</sub>/<i>a</i>) with a random distribution of Li<sup>+</sup>(Na<sup>+</sup>), Gd<sup>3+</sup>, and vacancies in the crystal. A Na<sub>2/7</sub>Gd<sub>4/7</sub>MoO<sub>4</sub> single crystal with scheelite-type structure has been grown by the Czochralski method. Transmission electron microscopy revealed that Na<sub>2/7</sub>Gd<sub>4/7</sub>MoO<sub>4</sub> has a (3 + 2)­D incommensurately modulated structure. The (3 + 2)­D incommensurately modulated scheelite-type cation-deficient structure of Na<sub>2/7</sub>Gd<sub>4/7</sub>MoO<sub>4</sub> [super space group <i>I</i>4̅ (α–β0,βα0)­00] has been solved from single-crystal diffraction data. The solution of the (3 + 2)­D incommensurately modulated structure revealed the partially disordered distribution of vacancies and Na and Gd cations. High-temperature conductivity measurements performed along the [100] and [001] orientation of the single crystal revealed that the conductivity of Na<sub>2/7</sub>Gd<sub>4/7</sub>MoO<sub>4</sub> at <i>T</i> = 973 K equals σ = 1.13 × 10<sup>–5</sup> Ω<sup>–1</sup> cm<sup>–1</sup>

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