scholarly journals Picosecond Acoustics Technique to Measure the Sound Velocities of Fe-Si Alloys and Si Single-Crystals at High Pressure

Minerals ◽  
2020 ◽  
Vol 10 (3) ◽  
pp. 214 ◽  
Author(s):  
Eric Edmund ◽  
Michel Gauthier ◽  
Daniele Antonangeli ◽  
Simon Ayrinhac ◽  
Silvia Boccato ◽  
...  

We describe here a time resolved pump-probe laser technique—picosecond interferometry—which has been combined with diamond anvil cells (DAC). This method enables the measurement of the longitudinal sound velocity up to Mbar pressure for any kind of material (solids, liquids, metals, insulators). We also provide a description of picosecond acoustics data analysis in order to determine the complete set of elastic constants for single crystals. To illustrate such capabilities, results are given on the pressure dependence of the acoustic properties for prototypical cases: polycrystal (hcp-Fe-5 wt% Si up to 115 GPa) and single-crystal (Si up to 10 GPa).

2009 ◽  
Author(s):  
Jie Zhang ◽  
A. Belousov ◽  
S. Katrych ◽  
J. Jun ◽  
J. Karpinski ◽  
...  

2005 ◽  
Vol 76 (11) ◽  
pp. 114301 ◽  
Author(s):  
Anchi Yu ◽  
Xiong Ye ◽  
Dan Ionascu ◽  
Wenxiang Cao ◽  
Paul M. Champion

2001 ◽  
Vol 6 (4) ◽  
pp. 235-237 ◽  
Author(s):  
Christopher D. Lane ◽  
David J. Hathcock ◽  
Andrew J. Leavitt ◽  
Farooq A. Khan ◽  
John E. Hansen

2013 ◽  
Vol 554-557 ◽  
pp. 1592-1601
Author(s):  
Severine A.E. Boyer ◽  
Jean Marc Haudin

A comprehensive understanding of the inherent link between in-situ growth kinetics of a polymer spherulite and high-pressure constraints under controlled temperature is concerned. As a matter of fact, while the link with temperature is well illustrated, little comprehensive study has been conducted to quantify the effect of pressure. This is yet required to model ‘extreme’ polymer processing conditions.Mainly, the experimental set-ups developed to reproduce the pressure effect can be classified into four families: “simple” cells, dilatometric set-ups, differential thermal analysis and diamond anvil plus in-situ measurement. In this context, an original model experiment, named CRISTAPRESS, has been constructed. The cell design exploits the optical properties of semi-crystalline spherulites. Time-resolved light depolarizing microscopic observations are conducted concomitantly with a fine PVT control, for high pressure up to 200 MPa and temperature up to 300 °C. The physical analysis of isothermal and isobaric holding of a model polymer shows the influence of temperature and pressure on the key kinetic parameters of crystallization, i.e., the growth rate and the number of activated nuclei, as well as on the subsequent morphologies. Simple modeling dealing with the Avrami equation and the Hoffman & Lauritzen theory is established.


1999 ◽  
Vol 32 (5) ◽  
pp. 1021-1023 ◽  
Author(s):  
Andrzej Katrusiak

Preparation of gaskets for high-pressure diffraction studies can be considerably facilitated by modifying the procedure of loading single crystals or powders into diamond-anvil cells. An effective procedure of pre-indenting gaskets after drilling the holes and a simple spark eroder for preparing the gaskets in the laboratory are described.


2002 ◽  
Vol 58 (6) ◽  
pp. 939-947 ◽  
Author(s):  
A. Pavlovska ◽  
S. Werner ◽  
B. Maximov ◽  
B. Mill

The hydrostatic compression of piezoelectric single crystals of La3Nb0.5Ga5.5O14 (LNG) and La3Ta0.5Ga5.5O14 (LTG) was studied at pressures of up to 23 GPa in diamond-anvil high-pressure cells using single-crystal X-ray diffraction techniques. The reflection-intensity data for LNG and LTG were collected at pressures of up to 22.8 GPa and 16.7 GPa, respectively. Both compounds show anisotropic behaviour under pressure, which is caused by differences in bonding parallel to the a and c directions. The compression of strongly rigid structures leads to increasing internal strains and results, at pressures of 12.4 (3) GPa for LNG and 11.7 (3) GPa for LTG, in a transition to lower symmetry. The compressibilities along the c axis are almost the same for LNG and LTG through the whole investigated pressure range. In contrast, the pressure dependencies of the a axis of these materials are similar only for the initial phase, and the axial compressibilities for the high-pressure polymorphs of LNG and LTG are significantly different to each other. The volume compressibilities of trigonal LNG and LTG (space group P321) are about 0.007 GPa−1; respective bulk moduli are 145 (3) GPa and 144 (2) GPa. The monoclinic high-pressure phases (space group A2) of LNG and LTG show differing compressions, which can be explained by the substitution of Ta5+ for Nb5+. Thus, the bulk moduli for the high-pressure polymorphs of LNG and LTG are B 0 = 93 (2) GPa and B 0 = 128 (12) GPa, respectively. The volume compressibilities of the high-pressure phases at 0.011 GPa−1 for LNG and 0.008 GPa−1 for LTG are higher than the initial phases, this effect being more pronounced in the case of LNG.


2011 ◽  
Vol 110 (11) ◽  
pp. 113112 ◽  
Author(s):  
Jie Zhang ◽  
Andrey Belousov ◽  
Janusz Karpiński ◽  
Bertram Batlogg ◽  
Gary Wicks ◽  
...  

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