<p>Leucite (ideally K[AlSi₂O₆]) exhibits a complex sequence of structural transformations upon heating, the nature of which—particularly the existence of intermediate phases and the behaviour of the extra-framework potassium cation—has long been debated. In this study, highly accurate in-situ high-temperature powder X-ray diffraction (HT-PXRD) data were collected over the 303–1173&#xa0;K range and analysed using the Rietveld method. The results support a continuous transition sequence from the low-temperature tetragonal <i>I</i>4<sub>1</sub>/<i>a</i> phase to an intermediate tetragonal <i>I</i>4<sub>1</sub>/<i>acd</i> modification, followed by the high-temperature cubic <i>Ia</i><InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\:\stackrel{-}{3}\)</EquationSource> </InlineEquation><i>d</i> phase. In the 873–898&#xa0;K interval, the data are best described by the coexistence of two phases, namely <i>I</i>4<sub>1</sub>/<i>a</i> + <i>I</i>4<sub>1</sub>/<i>acd</i> at 873&#xa0;K and <i>I</i>4<sub>1</sub>/<i>acd</i> + <i>Ia</i><InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\:\stackrel{-}{3}\)</EquationSource> </InlineEquation><i>d</i> at 898&#xa0;K. Given the long acquisition times and adequate thermal equilibration, the observed coexistence is best attributed to minor thermal gradients along the capillary rather than sluggish transition kinetics, providing a consistent explanation for previously reported lattice volume discontinuities. Furthermore, spontaneous strain analysis confirms that the ferroelastic transition is fully consistent, within experimental uncertainty, with a second-order Landau free energy expansion. While the intrinsic limitations of conventional PXRD preclude the refinement of Al/Si ordering, structural data indicate that the framework evolution is closely coupled to the extra-framework K cation. Bond-valence analysis indicates an apparent underbonding of K throughout the investigated range; however, this is consistent with pronounced dynamic disorder (rattling) within the framework cavities, prior to attaining a more regular 12-fold coordination in the cubic phase.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Phase transitions and structural evolution of leucite (K[AlSi₂O₆]) from in-situ high-temperature powder X-ray diffraction

  • Paolo Ballirano

摘要

Leucite (ideally K[AlSi₂O₆]) exhibits a complex sequence of structural transformations upon heating, the nature of which—particularly the existence of intermediate phases and the behaviour of the extra-framework potassium cation—has long been debated. In this study, highly accurate in-situ high-temperature powder X-ray diffraction (HT-PXRD) data were collected over the 303–1173 K range and analysed using the Rietveld method. The results support a continuous transition sequence from the low-temperature tetragonal I41/a phase to an intermediate tetragonal I41/acd modification, followed by the high-temperature cubic Ia \(\:\stackrel{-}{3}\) d phase. In the 873–898 K interval, the data are best described by the coexistence of two phases, namely I41/a + I41/acd at 873 K and I41/acd + Ia \(\:\stackrel{-}{3}\) d at 898 K. Given the long acquisition times and adequate thermal equilibration, the observed coexistence is best attributed to minor thermal gradients along the capillary rather than sluggish transition kinetics, providing a consistent explanation for previously reported lattice volume discontinuities. Furthermore, spontaneous strain analysis confirms that the ferroelastic transition is fully consistent, within experimental uncertainty, with a second-order Landau free energy expansion. While the intrinsic limitations of conventional PXRD preclude the refinement of Al/Si ordering, structural data indicate that the framework evolution is closely coupled to the extra-framework K cation. Bond-valence analysis indicates an apparent underbonding of K throughout the investigated range; however, this is consistent with pronounced dynamic disorder (rattling) within the framework cavities, prior to attaining a more regular 12-fold coordination in the cubic phase.