首页> 外文期刊>International Journal of Quantum Chemistry >Crystal structures and ionic conductivities of ternary derivatives of the silver and copper monohalides - I. Superionic phases of stoichiometry MA(4)I(5): RbAg4I5, KAg4I5, and KCu4I5
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Crystal structures and ionic conductivities of ternary derivatives of the silver and copper monohalides - I. Superionic phases of stoichiometry MA(4)I(5): RbAg4I5, KAg4I5, and KCu4I5

机译:银和铜一卤化物三元衍生物的晶体结构和离子电导率-I.化学计量比的超离子相MA(4)I(5):RbAg4I5,KAg4I5和KCu4I5

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The superionic properties of the compounds RbAg4I5, KAg4I5 and KCu4I5, have been investigated by powder neutron diffraction and complex impedance spectroscopy. RbAg4I5 and KAg4I5 have room-temperature ionic conductivities of sigma = 0.21(6) and 0.08(5) Omega(-1) cm(-1), respectively, which increase gradually on increasing temperature. KCu4I5 is only stable in the temperature range between 515(5) K and its melting point of 605 K, and its ionic conductivity is sigma = 0.61(8) Omega(-1) cm(-1), at T = 540 K. At lower temperatures, KCu4I5 disproportionates into KI + 4CuI and the ionic conductivity falls by over three orders of magnitude. Least-squares refinements of the powder neutron diffraction data for RbAg4I5 at ambient temperature confirm the reported structure (space group P4(1)32, Z = 4, a = 11.23934(3) Angstrom), though with some differences in the preferred locations of the mobile Ag+. KAg4I5 and KCu4I5 are found to adopt the same basic structure as RbAg4I5, with the I- forming a beta-Mn-type sublattice, with the K+ located in a distorted octahedral environment and the Ag+(Cu+) predominantly distributed over two sites which are tetrahedrally co-ordinated to V. The implications for the conduction mechanism within these compounds are discussed, using a novel maximum entropy difference Fourier technique to map the distribution of the Ag+(Cu+) within the unit cell. (C) 2002 Elsevier Science (USA). [References: 27]
机译:化合物RbAg4I5,KAg4I5和KCu4I5的超离子性质已通过粉末中子衍射和复阻抗谱研究。 RbAg4I5和KAg4I5的室温离子电导率分别为sigma = 0.21(6)和0.08(5)Omega(-1)cm(-1),随着温度的升高而逐渐增加。 KCu4I5仅在515(5)K至605 K的熔点之间的温度范围内稳定,其离子电导率在T = 540 K时为sigma = 0.61(8)Omega(-1)cm(-1)。在较低温度下,KCu4I5歧化为KI + 4CuI,离子电导率下降了三个数量级以上。 RbAg4I5在环境温度下的粉末中子衍射数据的最小二乘法改进证实了所报道的结构(空间群P4(1)32,Z = 4,a = 11.23934(3)埃),尽管在移动式Ag +。发现KAg4I5和KCu4I5采用与RbAg4I5相同的基本结构,其中I-形成β-Mn型亚晶格,K +位于扭曲的八面体环境中,而Ag +(Cu +)主要分布在两个四面体位置使用新颖的最大熵差傅里叶技术绘制了Ag +(Cu +)在晶胞内的分布图,讨论了这些化合物中传导机理的含义。 (C)2002 Elsevier Science(美国)。 [参考:27]

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