Chang Hong-Young, Kim Sang-Hwan, Halasyamani P Shiv, Ok Kang Min
Department of Chemistry, University of Houston, 136 Fleming Building, Houston, Texas 77204-5003, USA.
J Am Chem Soc. 2009 Feb 25;131(7):2426-7. doi: 10.1021/ja808469a.
A new polar noncentrosymmetric material, Li(2)Ti(IO(3))(6), has been synthesized and characterized. The material is built up from a TiO(6) octahedron that is linked to six IO(3) polyhedra. These polyhedral groups are separated by Li(+) cations. The Ti(4+) and I(5+) cations are in asymmetric polar coordination environments attributable to second-order Jahn-Teller effects. The distortion associated with the Ti(4+) cation is negligible, since the TiO(6) octahedra are completely surrounded by IO(3) polyhedra. The I(5+) cation is in a highly polar asymmetric coordination environment attributable to its stereoactive lone pair, which was qualitatively described by pseudopotential calculations of the electron localization function. The macroscopic polarity of Li(2)Ti(IO(3))(6) may be attributed to parallel alignment of the stereoactive lone pairs on the I(5+) cations. This parallel alignment profoundly influences the material's functional properties: second-harmonic generation, piezoelectricity, and pyroelectricity. The material is, however, not ferroelectric, as the polarization associated with I(5+) is not switchable.
一种新型极性非中心对称材料Li₂Ti(IO₃)₆已被合成并表征。该材料由一个与六个IO₃多面体相连的TiO₆八面体构成。这些多面体基团被Li⁺阳离子隔开。Ti⁴⁺和I⁵⁺阳离子处于归因于二阶 Jahn - Teller效应的不对称极性配位环境中。与Ti⁴⁺阳离子相关的畸变可忽略不计,因为TiO₆八面体完全被IO₃多面体包围。I⁵⁺阳离子处于高度极性的不对称配位环境中,这归因于其立体活性孤对电子,电子定位函数的赝势计算对其进行了定性描述。Li₂Ti(IO₃)₆的宏观极性可能归因于I⁵⁺阳离子上立体活性孤对电子的平行排列。这种平行排列深刻影响材料的功能特性:二次谐波产生、压电性和热电性。然而,该材料不是铁电体,因为与I⁵⁺相关的极化不可切换。