Crystal Structures and Phase Transitions in A-Site Deficient Perovskites Ln1/3TaO3

2008 ◽  
Vol 20 (21) ◽  
pp. 6666-6676 ◽  
Author(s):  
Qingdi Zhou ◽  
Paul J. Saines ◽  
Neeraj Sharma ◽  
Jimmy Ting ◽  
Brendan J. Kennedy ◽  
...  
ChemInform ◽  
2009 ◽  
Vol 40 (6) ◽  
Author(s):  
Qingdi Zhou ◽  
Paul J. Saines ◽  
Neeraj Sharma ◽  
Jimmy Ting ◽  
Brendan J. Kennedy ◽  
...  

2021 ◽  
Vol 103 (6) ◽  
Author(s):  
J. Blasco ◽  
G. Subías ◽  
M. L. Sanjuán ◽  
J. L. García-Muñoz ◽  
F. Fauth ◽  
...  

ChemBioChem ◽  
2003 ◽  
Vol 4 (10) ◽  
pp. 1078-1088 ◽  
Author(s):  
Peter Pfister ◽  
Sven Hobbie ◽  
Quentin Vicens ◽  
Erik C. Böttger ◽  
Eric Westhof

2011 ◽  
Vol 26 (2) ◽  
pp. 119-125 ◽  
Author(s):  
Sytle M. Antao ◽  
Ishmael Hassan

The crystal structures of marialite (Me6) from Badakhshan, Afghanistan and meionite (Me93) from Mt. Vesuvius, Italy were obtained using synchrotron high-resolution powder X-ray diffraction (HRPXRD) data and Rietveld structure refinements. Their structures were refined in space groups I4/m and P42/n, and similar results were obtained. The Me6 sample has a formula Ca0.24Na3.37K0.24[Al3.16Si8.84O24]Cl0.84(CO3)0.15, and its unit-cell parameters are a=12.047555(7), c=7.563210(6) Å, and V=1097.751(1) Å3. The average ⟨T1-O⟩ distances are 1.599(1) Å in I4/m and 1.600(2) Å in P42/n, indicating that the T1 site contains only Si atoms. In P42/n, the average distances of ⟨T2-O⟩=1.655(2) and ⟨T3-O⟩=1.664(2) Å are distinct and are not equal to each other. However, the mean ⟨T2,3-O⟩=1.659(2) Å in P42/n and is identical to the ⟨T2′-O⟩=1.659(1) Å in I4/m. The ⟨M-O⟩ [7]=2.754(1) Å (M site is coordinated to seven framework O atoms) and M-A=2.914(1) Å; these distances are identical in both space groups. The Me93 sample has a formula of Na0.29Ca3.76[Al5.54Si6.46O24]Cl0.05(SO4)0.02(CO3)0.93, and its unit-cell parameters are a=12.19882(1), c=7.576954(8) Å, and V=1127.535(2) Å3. A similar examination of the Me93 sample also shows that both space groups give similar results; however, the C–O distance is more reasonable in P42/n than in I4/m. Refining the scapolite structure near Me0 or Me100 in I4/m forces the T2 and T3 sites (both with multiplicity 8 in P42/n) to be equivalent and form the T2′ site (with multiplicity 16 in I4/m), but ⟨T2-O⟩ is not equal to ⟨T3-O⟩ in P42/n. Using different space groups for different regions across the series implies phase transitions, which do not occur in the scapolite series.


2018 ◽  
Vol 5 (3) ◽  
pp. 619-625 ◽  
Author(s):  
Ying Liu ◽  
Maxim S. Molokeev ◽  
Quanlin Liu ◽  
Zhiguo Xia

Structures and phase transitions depending on compositions and temperature between R3̄c and R3̄ in Na(2−2x)Srx[ ]xZr4(PO4)6 have been investigated.


Author(s):  
Dušica Jovanović ◽  
Dejan Zagorac ◽  
Branko Matović ◽  
Aleksandra Zarubica ◽  
Jelena Zagorac

Recent studies of TiO2/TiS2 nanostructures with various morphologies have been reported, usually showing improved properties with applications from electronics and catalysis to solar cells and medicine. However, there is a limited number of studies on the crystal structures of TiO2/TiS2 compounds with corresponding properties. In this research, relevant crystal structures of TiO1–x S x (x = 0, 0.25, 0.5, 0.75 and 1) solid solutions were investigated using an ab initio method. For each composition, crystal structures adopting anatase, rutile and CdI2 structure type were calculated on LDA-PZ and GGA-PBE levels of theory. Novel phase transitions and predicted structures are presented, and apart from several interesting metastable structures, a very interesting pressure-induced phase transition is found in the TiOS compound. Furthermore, electronic properties were studied through the dependence of semiconducting properties on dopant concentration. The first description of the electronic properties of the mixed TiO1–x S x compounds in crystal form has been presented, followed by a detailed study of the structure–property relationship, which will possibly have numerous industrial and technological applications.


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