3 research outputs found

    Unraveling Hidden Mg–Mn–H Phase Relations at High Pressures and Temperatures by <i>in Situ</i> Synchrotron Diffraction

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    The Mg–Mn–H system was investigated by <i>in situ</i> high pressure studies of reaction mixtures MgH<sub>2</sub>–Mn–H<sub>2</sub>. The formation conditions of two complex hydrides with composition Mg<sub>3</sub>MnH<sub>7</sub> were established. Previously known hexagonal Mg<sub>3</sub>MnH<sub>7</sub> (h-Mg<sub>3</sub>MnH<sub>7</sub>) formed at pressures 1.5–2 GPa and temperatures between 480 and 500 °C, whereas an orthorhombic form (o-Mg<sub>3</sub>MnH<sub>7</sub>) was obtained at pressures above 5 GPa and temperatures above 600 °C. The crystal structures of the polymorphs feature octahedral [Mn­(I)­H<sub>6</sub>]<sup>5–</sup> complexes and interstitial H<sup>–</sup>. Interstitial H<sup>–</sup> is located in trigonal bipyramidal and square pyramidal interstices formed by Mg<sup>2+</sup> ions in h- and o-Mg<sub>3</sub>MnH<sub>7</sub>, respectively. The hexagonal form can be retained at ambient pressure, whereas the orthorhombic form upon decompression undergoes a distortion to monoclinic Mg<sub>3</sub>MnH<sub>7</sub> (m-Mg<sub>3</sub>MnH<sub>7</sub>). The structure elucidation of o- and m-Mg<sub>3</sub>MnH<sub>7</sub> was aided by first-principles density functional theory (DFT) calculations. Calculated enthalpy versus pressure relations predict m- and o-Mg<sub>3</sub>MnH<sub>7</sub> to be more stable than h-Mg<sub>3</sub>MnH<sub>7</sub> above 4.3 GPa. Phonon calculations revealed o-Mg<sub>3</sub>MnH<sub>7</sub> to be dynamically unstable at pressures below 5 GPa, which explains its phase transition to m-Mg<sub>3</sub>MnH<sub>7</sub> on decompression. The electronic structure of the quenchable polymorphs h- and m-Mg<sub>3</sub>MnH<sub>7</sub> is very similar. The stable 18-electron complex [MnH<sub>6</sub>]<sup>5–</sup> is mirrored in the occupied states, and calculated band gaps are around 1.5 eV. The study underlines the significance of <i>in situ</i> investigations for mapping reaction conditions and understanding phase relations for hydrogen-rich complex transition metal hydrides

    Unraveling Hidden Mg–Mn–H Phase Relations at High Pressures and Temperatures by <i>in Situ</i> Synchrotron Diffraction

    No full text
    The Mg–Mn–H system was investigated by <i>in situ</i> high pressure studies of reaction mixtures MgH<sub>2</sub>–Mn–H<sub>2</sub>. The formation conditions of two complex hydrides with composition Mg<sub>3</sub>MnH<sub>7</sub> were established. Previously known hexagonal Mg<sub>3</sub>MnH<sub>7</sub> (h-Mg<sub>3</sub>MnH<sub>7</sub>) formed at pressures 1.5–2 GPa and temperatures between 480 and 500 °C, whereas an orthorhombic form (o-Mg<sub>3</sub>MnH<sub>7</sub>) was obtained at pressures above 5 GPa and temperatures above 600 °C. The crystal structures of the polymorphs feature octahedral [Mn­(I)­H<sub>6</sub>]<sup>5–</sup> complexes and interstitial H<sup>–</sup>. Interstitial H<sup>–</sup> is located in trigonal bipyramidal and square pyramidal interstices formed by Mg<sup>2+</sup> ions in h- and o-Mg<sub>3</sub>MnH<sub>7</sub>, respectively. The hexagonal form can be retained at ambient pressure, whereas the orthorhombic form upon decompression undergoes a distortion to monoclinic Mg<sub>3</sub>MnH<sub>7</sub> (m-Mg<sub>3</sub>MnH<sub>7</sub>). The structure elucidation of o- and m-Mg<sub>3</sub>MnH<sub>7</sub> was aided by first-principles density functional theory (DFT) calculations. Calculated enthalpy versus pressure relations predict m- and o-Mg<sub>3</sub>MnH<sub>7</sub> to be more stable than h-Mg<sub>3</sub>MnH<sub>7</sub> above 4.3 GPa. Phonon calculations revealed o-Mg<sub>3</sub>MnH<sub>7</sub> to be dynamically unstable at pressures below 5 GPa, which explains its phase transition to m-Mg<sub>3</sub>MnH<sub>7</sub> on decompression. The electronic structure of the quenchable polymorphs h- and m-Mg<sub>3</sub>MnH<sub>7</sub> is very similar. The stable 18-electron complex [MnH<sub>6</sub>]<sup>5–</sup> is mirrored in the occupied states, and calculated band gaps are around 1.5 eV. The study underlines the significance of <i>in situ</i> investigations for mapping reaction conditions and understanding phase relations for hydrogen-rich complex transition metal hydrides

    Understanding Antiferromagnetic Coupling in Lead-Free Halide Double Perovskite Semiconductors

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    Solution-processable semiconductors with antiferromagnetic (AFM) order are attractive for future spintronics and information storage technology. Halide perovskites containing magnetic ions have emerged as multifunctional materials, demonstrating a cross-link between structural, optical, electrical, and magnetic properties. However, stable optoelectronic halide perovskites that are antiferromagnetic remain sparse, and the critical design rules to optimize magnetic coupling still must be developed. Here, we combine the complementary magnetometry and electron-spin-resonance experiments, together with first-principles calculations to study the antiferromagnetic coupling in stable Cs2(Ag:Na)FeCl6 bulk semiconductor alloys grown by the hydrothermal method. We show the importance of nonmagnetic monovalence ions at the BI site (Na/Ag) in facilitating the superexchange interaction via orbital hybridization, offering the tunability of the Curie–Weiss parameters between −27 and −210 K, with a potential to promote magnetic frustration via alloying the nonmagnetic BI site (Ag:Na ratio). Combining our experimental evidence with first-principles calculations, we draw a cohesive picture of the material design for B-site-ordered antiferromagnetic halide double perovskites
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