| People | Locations | Statistics |
|---|---|---|
| Naji, M. |
| |
| Motta, Antonella |
| |
| Aletan, Dirar |
| |
| Mohamed, Tarek |
| |
| Ertürk, Emre |
| |
| Taccardi, Nicola |
| |
| Kononenko, Denys |
| |
| Petrov, R. H. | Madrid |
|
| Alshaaer, Mazen | Brussels |
|
| Bih, L. |
| |
| Casati, R. |
| |
| Muller, Hermance |
| |
| Kočí, Jan | Prague |
|
| Šuljagić, Marija |
| |
| Kalteremidou, Kalliopi-Artemi | Brussels |
|
| Azam, Siraj |
| |
| Ospanova, Alyiya |
| |
| Blanpain, Bart |
| |
| Ali, M. A. |
| |
| Popa, V. |
| |
| Rančić, M. |
| |
| Ollier, Nadège |
| |
| Azevedo, Nuno Monteiro |
| |
| Landes, Michael |
| |
| Rignanese, Gian-Marco |
|
Bouvier, Pierre
Institut Néel
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (24/24 displayed)
- 2023VO2 under hydrostatic pressure: Isostructural phase transition close to a critical end-pointcitations
- 2019Three-phase metal-insulator transition and structural alternative for a VO2 film epitaxially grown on Al2O3(0001)citations
- 2015High pressure single crystal x-ray and neutron powder diffraction study of the ferroelectric-paraelectric phase transition in PbTiO3citations
- 2014Jahn-Teller, Polarity, and Insulator-to-Metal Transition in BiMnO3 at High Pressurecitations
- 2012X-ray diffraction from stishovite under nonhydrostatic compression to 70 GPa: Strength and elasticity across the tetragonal → orthorhombic transitioncitations
- 2011High-pressure polarized Raman spectra of Gd(2)(MoO(4))(3): phase transitions and amorphizationcitations
- 2010Absence of pressure-induced amorphization in LiKSO4citations
- 2010Pressure-temperature phase diagram of SrTiO3 up to 53 GPacitations
- 2009Single crystal growth of BiMnO3 under high pressure-high temperature
- 2007Comparative study and imaging by PhotoElectroChemical techniques of oxide films thermally grown on zirconium and Zircaloy-4citations
- 2007Structural evolution of (Ca 0.35 Sr 0.65 )TiO 3 perovskite at high pressurescitations
- 2006Hot compaction of nanocrystalline TiO<sub>2</sub> (anatase) ceramics. Mechanisms of densification: Grain size and doping effectscitations
- 2006Raman scattering of the model multiferroic oxide BiFeO 3 : effect of temperature, pressure and stresscitations
- 2006Raman scattering of the model multiferroic oxide BiFeO<sub>3</sub>: effect of temperature, pressure and stresscitations
- 2006SnO 2 /MoO 3 -nanostructure and alcohol detectioncitations
- 2006Raman Imaging and Kelvin Probe Microscopy for the Examination of the Heterogeneity of Doping in Polycrystalline Boron-Doped Diamond Electrodes
- 2006Raman spectroscopy of Cs<SUB>2</SUB>HgBr<SUB>4</SUB> at high-pressure: effect of hydrostaticitycitations
- 2006Raman spectroscopy of Cs 2 HgBr 4 at high-pressure: effect of hydrostaticitycitations
- 2005The high-pressure structural phase transitions of sodium bismuth titanatecitations
- 2004Decomposition of LiGdF 4 scheelite at high pressurescitations
- 2003Quantification of Chemical Pressure in Doped Nanostructured Zirconia Ceramicscitations
- 2002X-ray diffraction study of WO 3 at high pressurecitations
- 2002X-ray diffraction study of WO<sub>3</sub> at high pressurecitations
- 2000Raman study of phases and stresses distributions in oxidation scales of Zirconim alloys: spectroscopic study of pressure and temperature effects on different nanometric Zirconia
Places of action
| Organizations | Location | People |
|---|
article
X-ray diffraction study of WO<sub>3</sub> at high pressure
Abstract
The high-pressure behaviour of microcrystalline tungsten oxide (WO<SUB>3</SUB>) has been investigated with angle-dispersive synchrotron x-ray powder diffraction in a diamond anvil cell up to 40 GPa at room temperature. Up to 21 GPa, the pressure dependence of the volume of the monoclinic high-pressure (<I>P</I>2<SUB>1</SUB>/<I>c</I>) phase is described by a third-order Birch–Murnaghan equation of state with parameters <I>V</I><SUB>0</SUB> = 210.9(7)Å<SUP>3</SUP>, <I>K</I><SUB><I>T</I></SUB> = 27(2)<I>GP</I> <I>a</I> and <I>K</I>' = 9.4(5). At 24 GPa, a first-order phase transition occurs with an approximate Δ<I>V</I> of 7.4% to a monoclinic <I>P</I>2<SUB>1</SUB>/<I>a</I> unit cell with <I>a</I> = 6.1669(8)Å, <I>b</I> = 4.5758(6)Å, <I>c</I> = 5.3159(6)Å, β = 101.440(9)<SUP>ˆ</SUP>. A second transition is observed at pressures higher than 31 GPa with an approximate Δ<I>V</I> of 12% to a phase described by a third monoclinic unit cell, with <I>a</I> = 10.3633(22)Å, <I>b</I> = 3.9065(8)Å, <I>c</I> = 9.3459(18)Å and β = 98.539(14)ˆ