Lanthanum (Oxo)nitridosilicates: From Ordered to Disordered Crystal Structures

2015 ◽  
Vol 642 (2) ◽  
pp. 101-106 ◽  
Author(s):  
Dajana Durach ◽  
Wolfgang Schnick
1968 ◽  
Vol 12 ◽  
pp. 23-49 ◽  
Author(s):  
Bill C. Giessen

AbstractThe crystal structures of elements and alloy phases in the B-metal region (B2(Zn) to B5(As) groups) have been classified into phase fields determined by their position in the periodic table. The limited number of equilibrium phases with element-like, disordered crystal structures and of extended terminal solid solutions has been more than doubled by the addition of metastable phases produced by ultra-rapid quenching from the melt (splat cooling). Strong structural correlations exist. Some high pressure phases have been included; in some cases, a qualitative discussion from the viewpoint of pseudopotential theory is given.


IUCrJ ◽  
2021 ◽  
Vol 8 (2) ◽  
pp. 305-318 ◽  
Author(s):  
Birger Dittrich

Distinguishing disorder into static and dynamic based on multi-temperature X-ray or neutron diffraction experiments is the current state of the art, but is only descriptive, not predictive. Here, several disordered structures are revisited from the Cambridge Crystallographic Data Center `drug subset', the Cambridge Structural Database and own earlier work, where experimental intensities of Bragg diffraction data were available. Using the molecule-in-cluster approach, structures with distinguishable conformations were optimized separately, as extracted from available or generated disorder models of the respective disordered crystal structures. Re-combining these `archetype structures' by restraining positional and constraining displacement parameters for conventional least-squares refinement, based on the optimized geometries, then often achieves a superior fit to the experimental diffraction data compared with relying on experimental information alone. It also simplifies and standardizes disorder refinement. Ten example structures were analysed. It is observed that energy differences between separate disorder conformations are usually within a small energy window of RT (T = crystallization temperature). Further computations classify disorder into static or dynamic, using single experiments performed at one single temperature, and this was achieved for propionamide.


1997 ◽  
Vol 134 (1) ◽  
pp. 164-169 ◽  
Author(s):  
D.J. Williams ◽  
D.E. Partin ◽  
F.J. Lincoln ◽  
J. Kouvetakis ◽  
M. O'Keeffe

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