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Polar Hexagonal Tungsten Oxide (HTO) Materials: (1) Synthesis, Characterization, Functional Properties, and Structure−Property Relationships in A2(MoO3)3(SeO3) (A = Rb+ and Tl+) and (2) Classification, Structural Distortions, and Second-Harmonic Generating Properties of Known Polar HTOs

Two new polar noncentrosymmetric (NCS) oxides, Rb2(MoO3)3(SeO3) and Tl2(MoO3)3(SeO3), have been synthesized and characterized. The materials exhibit the layered hexagonal tungsten oxide (HTO) structural topologyClass 2, i.e., the MoO6 layers are “capped” on one side by the SeO3 polyhedra. The Rb+ a...

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Bibliographic Details
Published in:Chemistry of materials 2010-05, Vol.22 (10), p.3241-3250
Main Authors: Chang, Hong Young, Kim, Sun Woo, Halasyamani, P. Shiv
Format: Article
Language:English
Online Access:Get full text
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Summary:Two new polar noncentrosymmetric (NCS) oxides, Rb2(MoO3)3(SeO3) and Tl2(MoO3)3(SeO3), have been synthesized and characterized. The materials exhibit the layered hexagonal tungsten oxide (HTO) structural topologyClass 2, i.e., the MoO6 layers are “capped” on one side by the SeO3 polyhedra. The Rb+ and Tl+ cations are found between the layers. The Mo6+ and Se4+ cations are present in asymmetric coordination environments that are attributable to second-order Jahn−Teller (SOJT) effects. In addition to structural characterization, the materials were characterized by second-harmonic generation (SHG), piezoelectric, and polarization measurements. SHG measurements using 1064-nm radiation revealed doubling efficiencies of 300 and 400 × α-SiO2 for the Rb- and Tl-phases, respectively. Piezoelectric experiments revealed d 33 values of ∼9−13 pm/V. Polarization measurements indicate that the materials are not ferroelectric, i.e., the polarization is not “switchable”. The materials are pyroelectric, with total pyroelectric coefficients (p), at 45 °C, of −1.1 μC m−2 K−1 for Rb2(MoO3)3(SeO3) and −2.1 μC m−2 K−1 for Tl2(MoO3)3(SeO3). Thermogravimetry, differential scanning calorimetry, UV−vis, and infrared spectroscopy measurements were also performed. We also examine all of the known polar HTO-type materials to gain a better understanding of the functional properties and structure−property relationships. Crystal data for Rb2(MoO3)3(SeO3): hexagonal, space group P63 (No. 173), a = b = 7.2992(14) Å, c = 11.978(5) Å, V = 552.7(3) Å3, and Z = 2; crystal data for Tl2(MoO3)3(SeO3): trigonal, space group P31c (No. 159), a = b = 7.2867(10) Å, c = 11.794(3) Å, V = 542.33(18) Å3, and Z = 2.
ISSN:0897-4756
1520-5002
DOI:10.1021/cm100476m