National Renewable Energy Laboratory, Golden, Colorado 80401, USA.
J Am Chem Soc. 2011 Aug 3;133(30):11649-54. doi: 10.1021/ja2034602. Epub 2011 Jul 12.
The crystal structures of A(2)BO(4) spinel oxides are classified as either normal or inverse, representing different distributions of the A and B cations over the tetrahedrally and octahedrally coordinated cation sites. These structures undergo characteristic structural changes as a function of temperature: (i) the nominally disordered inverse structure orders crystallographically at low T, and (ii) at finite temperatures, both inverse and normal develop characteristic distributions of cations associated with order-disorder structural changes. We show here that all of these universal features emerge naturally from a simple point-ion electrostatic (PIE) model with a single adjustable parameter. Monte Carlo simulations of the PIE Hamiltonian provide quantitative order-disorder characteristic temperatures. We show that, with the help of the PIE model, the magnitude of the temperatures can be inferred from the nominal charges of the atomic species in the spinel. Indeed, we show that characteristic order-disorder temperatures in 3-2 spinels (nominal charges Z(A) = 3 and Z(B) = 2) are approximately an order of magnitude lower than in 2-4 spinels, thus explaining why typical 3-2 samples exhibit much larger degrees of disorder than those belonging to the 2-4 class.
尖晶石 A(2)BO(4)氧化物的晶体结构分为正常尖晶石和反尖晶石,这代表了 A 和 B 阳离子在四面体和八面体配位阳离子位置上的不同分布。这些结构随温度呈现出特征性的结构变化:(i) 名义上无序的反尖晶石结构在低温下结晶学有序,以及 (ii) 在有限温度下,反尖晶石和正常尖晶石都发展出与有序-无序结构变化相关的特征阳离子分布。我们在这里表明,所有这些普遍特征都可以从一个具有单个可调参数的简单点离子静电 (PIE) 模型自然地出现。PIE 哈密顿量的蒙特卡罗模拟提供了定量的有序-无序特征温度。我们表明,借助 PIE 模型,可以从尖晶石中原子种类的名义电荷推断出温度的大小。事实上,我们表明,3-2 尖晶石(名义电荷 Z(A) = 3 和 Z(B) = 2)中的特征有序-无序温度大约低一个数量级,这解释了为什么典型的 3-2 样品表现出比属于 2-4 类的样品大得多的无序程度。