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dc.contributor.authorKennedy, Brendan James
dc.contributor.authorSaura-Múzquiz, Matilde
dc.contributor.authorMarlton, Frederick
dc.contributor.authorMullens, Bryce
dc.contributor.authorManjón-Sanz, Alicia María
dc.contributor.authorNeuefeind, Joerg C.
dc.contributor.authorEverett, Michelle
dc.contributor.authorBrand, Helen E. A.
dc.contributor.authorMondald, S.
dc.contributor.authorVaitheeswaran, G.
dc.date.accessioned2023-12-11T02:12:59Z
dc.date.available2023-12-11T02:12:59Z
dc.date.issued2022en
dc.identifier.urihttps://hdl.handle.net/2123/31968
dc.description.abstractThe stereochemical activity of lone pair electrons plays a central role in determining the structural and electronic properties of both chemically simple materials such as H2O, as well as more complex condensed phases such as photocatalysts or thermoelectrics. TlReO4 is a rare example of a non-magnetic material exhibiting a re-entrant phase transition and emphanitic behavior in the long-range structure. Here, we describe the role of the Tl+ 6s2 lone pair electrons in these unusual phase transitions and illustrate its tunability by chemical doping, which has broad implications for functional materials containing lone pair bearing cations. First-principles density functional calculations clearly show the contribution of the Tl+ 6s2 in the valence band region. Local structure analysis, via neutron total scattering, revealed that changes in the long-range structure of TlReO4 occur due to changes in the correlation length of the Tl+ lone pairs. This has a significant effect on the anion interactions, with long-range ordered lone pairs creating a more densely packed structure. This resulted in a trade-off between anionic repulsions and lone pair correlations that lead to symmetry lowering upon heating in the long-range structure, whereby lattice expansion was necessary for the Tl+ lone pairs to become highly correlated. Similarly, introducing lattice expansion through chemical pressure allowed long-range lone pair correlations to occur over a wider temperature range, demonstrating a method for tuning the energy landscape of lone pair containing functional materials.en
dc.language.isoenen
dc.publisherACSen
dc.relation.ispartofJournal of the American Chemical Societyen
dc.rightsOtheren
dc.subjectCationsen
dc.subjectChemical structureen
dc.subjectDopingen
dc.subjectElectronic structureen
dc.subjectPhase transitionsen
dc.titleUnderstanding the re-entrant phase transition in a non-magnetic scheeliteen
dc.typeArticleen
dc.identifier.doi10.1021/jacs.2c05620
dc.type.pubtypeAuthor accepted manuscripten
usyd.facultySeS faculties schools::Faculty of Science::School of Chemistryen
usyd.citation.volume144en
usyd.citation.issue34en
usyd.citation.spage15612en
usyd.citation.epage15621en
workflow.metadata.onlyNoen


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