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Synthesis, crystal structure and dielectric properties of C6H18N2SbCl5

机译:C6H18N2SbCl5的合成,晶体结构和介电性能

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The result of the X-ray diffraction, differential scanning calorimetry and dielectric studies on a new crystal material C6H18N2SbCl5 is presented. The new organic-inorganic compound has been synthesized and characterized by the X-ray diffraction method at 296(2) K. It crystallizes in the monoclinic P21 space group. The cell dimensions are: a = 5.8617(1), b = 15.7069(2) angstrom, c = 16.6693(2) angstrom, beta = 97.627(1)degrees and Z = 4. The crystal structure consists of a discrete ionic layer of (C6H18N2)(2+) cations and [SbCl5](2-) anions linked via simple and bifurcated N. H center dot center dot center dot Cl hydrogen bonds. DSC analysis shows that this compound undergoes a phase transition at about (384 +/- 2) K. AC and DC conductivities, complex dielectric permittivity e*(omega) and complex electrical modulus M*(omega) were respectively studied as temperature and frequency functions. The combined data support each other and confirm the existence of a structural phase transition at about 384 K. Moreover, the temperature dependence of the DC conductivity and relaxation frequency followed the Arrhenius relation. The frequency dependence of the real part of the AC conductivity in both phases follows the Jonscher's universal dynamic law: s' total sigma total (omega, T) = sigma'(DC)(T) + A(T).omega(s(T)). The behavior of s(T) with temperature suggests that the hopping over barrier model (CBH) and the small polaron tunneling mechanism (SPTM) prevail in phases I and II, respectively. Copyright (C) 2016 John Wiley & Sons, Ltd.
机译:介绍了一种新型晶体材料C6H18N2SbCl5的X射线衍射,差示扫描量热法和介电研究的结果。该新的有机-无机化合物已通过X射线衍射法在296(2)K下合成并表征。它在单斜P21 / n空间群中结晶。晶胞尺寸为:a = 5.8617(1),b = 15.7069(2)埃,c = 16.6693(2)埃,beta = 97.627(1)度,Z =4。晶体结构由一个离散的离子层组成(C6H18N2)(2+)阳离子和[SbCl5](2-)阴离子通过简单且分叉的N.H中心点中心点中心点C1氢键连接。 DSC分析表明,该化合物在大约(384 +/- 2)K时经历相变。分别研究了温度和频率下的交流和直流电导率,复介电常数e *ω和复数模量M *ω。功能。组合的数据相互支持,并确认在约384 K处存在结构相变。此外,DC电导率和弛豫频率的温度依赖性遵循Arrhenius关系。两相中交流电导率的实部的频率相关性均遵循Jonscher的通用动态定律:s的总sigma总和(omega,T)= sigma'(DC)(T)+ A(T).omega(s( T))。 s(T)随温度的变化表明,跃迁势垒模型(CBH)和小极化子隧穿机制(SPTM)分别在阶段I和阶段II中占主导地位。版权所有(C)2016 John Wiley&Sons,Ltd.

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