Antipolar 2D Metallicity with Tunable Valence W x+ (5 ≤ x ≤ 5.6) in the Layered Monophosphate Tungsten Bronzes [Ba(PO4)2]W m O3m–3

The newly discovered series of layered monophosphate tungsten bronzes (L-MPTB) [Ba­(PO4)2]­W m O3m–3 consist of m-layer-thick slabs of WO6 octahedra separated by barium-phosphate spacers. They display a 2D metallic behavior confined in the central part of the perovskite slabs. Here, we report the mi...

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Veröffentlicht in:Journal of the American Chemical Society 2024-08, Vol.146 (34), p.23955-23962
Hauptverfasser: Nimoh, Hicham, Arévalo-López, Angel M., Meier, Quintin N., Minaud, Claire, Huvé, Marielle, Capet, Frédéric, Cano, Andrés, Glaum, Robert, Mentré, Olivier
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Sprache:eng
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Zusammenfassung:The newly discovered series of layered monophosphate tungsten bronzes (L-MPTB) [Ba­(PO4)2]­W m O3m–3 consist of m-layer-thick slabs of WO6 octahedra separated by barium-phosphate spacers. They display a 2D metallic behavior confined in the central part of the perovskite slabs. Here, we report the missing m = 2 member of this series, containing the rather uncommon W5+ oxidation state. We have analyzed its structure-property relationships in relation to the other members of the L-MPTB family. In particular, we have determined its crystal structure by means of single-crystal X-ray and electron diffraction and investigated its physical properties from resistivity, Seebeck-coefficient and heat-capacity measurements combined with first-principles calculations. All the L-MPTB compounds show metallic behavior down to 1.8 K without any clear charge-density-wave (CDW) order. The m = 2 member, however, displays an increased influence of the spacer that translates into anisotropic negative thermal expansion, reversed thermopower and reversed crystal-field splitting of the tungsten t2g orbitals. Our analysis of the full [Ba­(PO4)2]­W m O3m–3 series reveals a systematic and significant W off-centering in their octahedral coordination. We identify the resulting anti-polar character of these W displacements as the crucial aspect behind the 2D metallicity of these systems: It leads to the presence of bound charges whose screening determines the distribution of mobile charges, tending to accumulate at the center of the [W m O3–m ] block. We argue that this mechanism is analogous to enhanced conductivity observed for charged domain walls in ferroelectrics, thus providing a general design rule to promote 2D metallicity in layered systems.
ISSN:0002-7863
1520-5126
DOI:10.1021/jacs.4c07022