Structural Phase Transitions in KTaO3:Li Crystals: Evidence from X-Ray Powder Diffraction Data

1996 ◽  
Vol 228-231 ◽  
pp. 633-638 ◽  
Author(s):  
S.A. Ivanov ◽  
V.V. Zhurov ◽  
G. Hermeler ◽  
Wulf Depmeier
Keyword(s):  
Phase Transitions ◽  
Powder Diffraction ◽  
Diffraction Data ◽  
Structural Phase ◽  
Powder Diffraction Data ◽  
Structural Phase Transitions ◽  
X Ray

Structural phase transitions in YPtGe2 and GdPtGe2

2018 ◽  
Vol 47 (17) ◽  
pp. 6075-6088 ◽  
Author(s):  
Oliver Janka ◽  
Rolf-Dieter Hoffmann ◽  
Birgit Heying ◽  
Rainer Pöttgen
Keyword(s):  
Phase Transitions ◽  
Single Crystal ◽  
Diffraction Data ◽  
Structural Phase ◽  
Structural Phase Transitions ◽  
X Ray Diffraction ◽  
Temperature Dependent ◽  
X Ray ◽  
Arc Melting

The germanides YPtGe2 and GdPtGe2 were synthesized from REGe2 precursor compounds and platinum by arc-melting and their structures were studied on the basis of temperature-dependent single crystal X-ray diffraction data.

Structural phase transitions of rubidiumpolyphosphate, Rb2{∞1} [P2O6]

1994 ◽  
Vol 209 (4) ◽  
Author(s):  
C. Holst ◽  
W. W. Schmahl ◽  
H. Fuess
Keyword(s):  
Phase Transitions ◽  
High Temperature ◽  
Powder Diffraction ◽  
Intermediate Phase ◽  
Structural Phase ◽  
Structural Phase Transitions ◽  
X Ray

AbstractHigh temperature X-ray powder diffraction measurements of rubidiumpolyphosphate, RbThe T→H transition shows a hysteresis of ca. 110 K and on cooling an intermediate phase, RbPO

Use of TALP with laboratory powder diffraction data from 2D detectors

2013 ◽  
Vol 28 (S2) ◽  
pp. S481-S490
Author(s):  
Oriol Vallcorba ◽  
Anna Crespi ◽  
Jordi Rius ◽  
Carles Miravitlles
Keyword(s):  
Organic Compounds ◽  
Structural Study ◽  
Powder Diffraction ◽  
Diffraction Data ◽  
Powder Pattern ◽  
Experimental Setup ◽  
Intensity Data ◽  
Powder Diffraction Data ◽  
X Ray ◽  
Molecular Compounds

The viability of the direct-space strategy TALP (Vallcorba et al., 2012b) to solve crystal structures of molecular compounds from laboratory powder diffraction data is shown. The procedure exploits the accurate metric refined from a ‘Bragg-Brentano’ powder pattern to extract later the intensity data from a second ‘texture-free’ powder pattern with the DAJUST software (Vallcorba et al., 2012a). The experimental setup for collecting this second pattern consists of a circularly collimated X-ray beam and a 2D detector. The sample is placed between two thin Mylar® foils, which reduces or even eliminates preferred orientation. With the combination of the DAJUST and TALP software a preliminary but rigorous structural study of organic compounds can be carried out at the laboratory level. In addition, the time-consuming filling of capillaries with diameters thinner than 0.3mm is avoided.

Temperature-induced structural phase transitions in RERhSn (RE = Y, Gd-Tm, Lu)

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Simon Engelbert ◽  
Rolf-Dieter Hoffmann ◽  
Jutta Kösters ◽  
Steffen Klenner ◽  
Rainer Pöttgen
Keyword(s):  
Rare Earth ◽  
Phase Transitions ◽  
Driving Force ◽  
Room Temperature ◽  
Structural Phase ◽  
Structural Phase Transitions ◽  
Line Broadening ◽  
X Ray Diffraction ◽  
Temperature Dependent ◽  
X Ray

Abstract The structures of the equiatomic stannides RERhSn with the smaller rare earth elements Y, Gd-Tm and Lu were reinvestigated on the basis of temperature-dependent single crystal X-ray diffraction data. GdRhSn crystallizes with the aristotype ZrNiAl at 293 and 90 K. For RE = Y, Tb, Ho and Er the HP-CeRuSn type (approximant with space group R3m) is already formed at room temperature, while DyRhSn adopts the HP-CeRuSn type below 280 K. TmRhSn and LuRhSn show incommensurate modulated variants with superspace groups P31m(1/3; 1/3; γ) 000 (No. 157.1.23.1) (γ = 3/8 for TmRhSn and γ = 2/5 for LuRhSn). The driving force for superstructure formation (modulation) is a strengthening of Rh–Sn bonding. The modulation is expressed in a 119Sn Mössbauer spectrum of DyRhSn at 78 K through line broadening.

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