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Synthesis of Na3WH9 and Na3ReH8 Ternary Hydrides at High Pressures

The Na–W–H and Na–Re–H ternary systems were studied in a diamond anvil cell through X-ray diffraction and Raman spectroscopy, supported by density functional theory and molecular dynamics calculations. Na3WH9 can be synthesized above 7.8 GPa and 1400 K, remaining stable between at least 0.1 and 42.1...

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Published in:Inorganic chemistry 2024-11, Vol.63 (45), p.21734-21741
Main Authors: Marqueño, Tomas, Osmond, Israel, Kuzovnikov, Mikhail A., Shuttleworth, Hannah A., Gallego-Parra, Samuel, Gregoryanz, Eugene, Hermann, Andreas, Howie, Ross T., Peña-Alvarez, Miriam
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container_issue 45
container_start_page 21734
container_title Inorganic chemistry
container_volume 63
creator Marqueño, Tomas
Osmond, Israel
Kuzovnikov, Mikhail A.
Shuttleworth, Hannah A.
Gallego-Parra, Samuel
Gregoryanz, Eugene
Hermann, Andreas
Howie, Ross T.
Peña-Alvarez, Miriam
description The Na–W–H and Na–Re–H ternary systems were studied in a diamond anvil cell through X-ray diffraction and Raman spectroscopy, supported by density functional theory and molecular dynamics calculations. Na3WH9 can be synthesized above 7.8 GPa and 1400 K, remaining stable between at least 0.1 and 42.1 GPa. The rhenium analogue Na3ReH8 can form at 10.1 GPa upon laser heating, being stable between at least 0.3 and 32.5 GPa. Na3WH9 and Na3ReH8 host [WH9]3– and [ReH8]3– anions, respectively, forming homoleptic 18-electron complexes in both cases. Both ternary hydrides show similar structural types and pressure dependent phase transitions. At the highest pressures they adopt a distorted fcc Heusler structure (Na3WH9–II′ and Na3ReH8–II′) while upon decompression the structure symmetrizes becoming fcc between ∼6.4 and 10 GPa for Na3WH9–II and at 17 GPa for Na3ReH8–II. On further pressure release, the fcc phases transform into variants of a (quasi-) hexagonal structure at ∼3 GPa, Na3WH9–I and Na3ReH8–I.
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title Synthesis of Na3WH9 and Na3ReH8 Ternary Hydrides at High Pressures
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