Diamond-Anvil Cell Observations of a New Methane Hydrate Phase in the 100-MPa Pressure Range

2001 ◽  
Vol 105 (19) ◽  
pp. 4664-4668 ◽  
Author(s):  
I-Ming Chou ◽  
Anurag Sharma ◽  
Robert C. Burruss ◽  
Russell J. Hemley ◽  
Alexander F. Goncharov ◽  
...  
2005 ◽  
Vol 19 (01n03) ◽  
pp. 335-337 ◽  
Author(s):  
C. Q. JIN ◽  
X. M. QIN ◽  
K. SHIMIZU ◽  
M. NISHIYAMA ◽  
T. NAMIKI ◽  
...  

The evolution of superconducting transition of CuBa 2 Ca 3 Cu 4 O 10+δ (i.e. Cu -1234) superconductor has been studied by using diamond anvil cell technique. The Tc of Cu -1234 can be enhanced continuously from ambient reaching to 123 K at 15 GPa. This seems the one more system besides Hg -12( n -1) n which demonstrate the positive pressure effect on Tc over a wide pressure range above 10 GPa.


2005 ◽  
Vol 19 (01n03) ◽  
pp. 259-261
Author(s):  
KATSUYA SHIMIZU

Experimental results in search for pressure-induced superconductivity are reviewed. Typical examples are simple inorganic and organic molecular crystals, magnetic metals, and elements. We have developed complex extreme condition of very low temperature down to 30 mK and ultra high pressure exceeding 200 GPa by assembling compact diamond-anvil cell (DAC) on a powerful 3 He /4 He dilution refrigerator. Using the newly developed apparatus and techniques, we have studied superconductivity in various materials in various pressure range. In this paper, we will shortly review our newly developed experimental apparatus and techniques and discuss about examples of pressure-induced superconductivity in simple metals.


2018 ◽  
Vol 115 (8) ◽  
pp. 1713-1717 ◽  
Author(s):  
Bing Li ◽  
Cheng Ji ◽  
Wenge Yang ◽  
Junyue Wang ◽  
Ke Yang ◽  
...  

The diamond anvil cell (DAC) is considered one of the dominant devices to generate ultrahigh static pressure. The development of the DAC technique has enabled researchers to explore rich high-pressure science in the multimegabar pressure range. Here, we investigated the behavior of the DAC up to 400 GPa, which is the accepted pressure limit of a conventional DAC. By using a submicrometer synchrotron X-ray beam, double cuppings of the beveled diamond anvils were observed experimentally. Details of pressure loading, distribution, gasket-thickness variation, and diamond anvil deformation were studied to understand the generation of ultrahigh pressures, which may improve the conventional DAC techniques.


1993 ◽  
Vol 26 (6) ◽  
pp. 843-845 ◽  
Author(s):  
P. Comodi ◽  
P. F. Zanazzi

The pressure sensor proposed by Shen, Gregorian & Holzapfel [High Press. Res. (1991), 7, 73–75], based on the pressure-dependent shift of the luminescence line due to the 5 D 0−7 F 0 electronic transition of Sm2+ in a matrix of BaFCl, has been tested in a diamond-anvil cell and calibrated against the R 1−R 2 doublet shift of ruby and the known NaCl equation of state, in the pressure range between 0.0001 and 4.3 GPa. The parabolic dependence of the shift from the pressure can be approximated by the equation Δ(nm) = 1.46P − 0.047P 2, where the shift, Δ, is in nm and the pressure, P, in GPa. The estimated error in the pressure measurements is 5%. The Sm2+: BaFCl luminescence sensor can be advantageously used in the low to moderate pressure range (0.0001–5 GPa or more).


2019 ◽  
Vol 11 ◽  
pp. 110001 ◽  
Author(s):  
Michael G. Pravica ◽  
Sarah Schyck ◽  
Blake Harris ◽  
Petrika Cifligu ◽  
Eunja Kim ◽  
...  

By irradiating a pressurized mixture of a fluorine-bearing compound ($XeF_2$) and $HgF_2$ with synchrotron hard x-rays (>7 keV) inside a diamond anvil cell, we have observed dramatic changes in the far-infrared spectrum within the 30-35 GPa pressure range which suggest that we may have formed $HgF_4$ in the following way: $XeF_2 \xrightarrow{hv} Xe + F_2$ (photochemically) and $HgF_2 + F_2 \rightarrow HgF_4$ (30 GPa < P < 35 GPa). This lends credence to recent theoretical calculations by Botana et al. that suggest that Hg may behave as a transition metal at high pressure in an environment with an excess of molecular fluorine. The spectral changes were observed to be reversible during pressure cycling above and below the above mentioned pressure range until a certain point when we suspect that molecular fluorine diffused out of the sample at lower pressure. Upon pressure release, $HgF_2$ and trace $XeF_2$ were observed to be remaining in the sample chamber suggesting that much of the $Xe$ and $F_2$ diffused and leaked out from the sample chamber.   Received: 29 October 2018,  Accepted: 18 January 2019; Edited by: A. Goñi, A. Cantarero, J. S. Reparaz; DOI: http://dx.doi.org/10.4279/PIP.110001 Cite as: M Pravica, S Schyck, B Harris, P Cifligu, E Kim, B Billinghurst, Papers in Physics 11, 110001 (2019). This paper, by M Pravica, S Schyck, B Harris, P Cifligu, E Kim, B Billinghurst, is licensed under the Creative Commons Attribution License 4.0.  


Minerals ◽  
2020 ◽  
Vol 10 (10) ◽  
pp. 877
Author(s):  
G. Diego Gatta ◽  
Davide Comboni ◽  
Paolo Lotti ◽  
Alessandro Guastoni ◽  
Nicola Rotiroti ◽  
...  

The high-pressure behavior of wardite, NaAl3(PO4)2(OH)4·2H2O (a = 7.0673(2) Å, c = 19.193(9) Å, Sp. Gr. P41212), has been investigated by in-situ single-crystal synchrotron diffraction experiments up to 9 GPa, using a diamond anvil cell under quasi-hydrostatic conditions. This phosphate does not experience any pressure-induced phase transition, or anomalous compressional behavior, within the pressure-range investigated: its compressional behavior is fully elastic and all the deformation mechanisms, at the atomic scale, are reversible upon decompression. A second-order Birch–Murnaghan Equation of State was fitted to the experimental data, weighted by their uncertainty in pressure (P) and volume (V), with the following refined parameters: V0 = 957.8(2) Å3 and KV0 = −V0(∂P/∂V)P0,T0 = 85.8(4) GPa (βV0 = 1/KV0 = 0.01166(5) GPa−1). Axial bulk moduli were also calculated, with: K0(a) = 98(3) GPa (β0(a) = 0.0034(1) GPa−1) and K0(c) = 64(1) GPa (β0(c) = 0.0052(1) GPa−1). The anisotropic compressional scheme is: K0(a):K0(c) = 1.53:1. A series of structure refinements were performed on the basis of the intensity data collected in compression and decompression. The mechanisms at the atomic scale, responsible for the structure anisotropy of wardite, are discussed.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Hirokazu Kadobayashi ◽  
Satoka Ohnishi ◽  
Hiroaki Ohfuji ◽  
Yoshitaka Yamamoto ◽  
Michihiro Muraoka ◽  
...  

AbstractHydrocarbon chemistry in the C–O–H system at high pressure and high temperature is important for modelling the internal structure and evolution of giant icy planets, such as Uranus and Neptune, as their interiors are thought to be mainly composed of water and methane. In particular, the formation of diamond from the simplest hydrocarbon, i.e., methane, under the internal conditions of these planets has been discussed for nearly 40 years. Here, we demonstrate the formation of diamond from methane hydrate up to 3800 K and 45 GPa using a CO2 laser-heated diamond anvil cell combined with synchrotron X-ray diffraction, Raman spectroscopy, and scanning electron microscopy observations. The results show that the process of dissociation and polymerisation of methane molecules to produce heavier hydrocarbons while releasing hydrogen to ultimately form diamond proceeds at milder temperatures (~ 1600 K) and pressures (13–45 GPa) in the C–O–H system than in the C–H system due to the influence of water. Our findings suggest that diamond formation can also occur in the upper parts of the icy mantles of giant icy planets.


1982 ◽  
Vol 36 (3) ◽  
pp. 302-306 ◽  
Author(s):  
Randal M. Hill ◽  
Sherril D. Christian

A technique has been developed for accurately inferring pressure in the diamond anvil cell in the relatively low pressure range of 0 to 6 kbar. The method is directly applicable to dilute solution studies using hydrocarbon solvents. A procedure is described for using the method with more concentrated solutions and with moderately polar organic solvents. The frequency shift of anthracene absorbance in five hydrocarbon solvents has been measured in the 0 to 2 kbar range and extended to 6 kbar. Pressures in this range were measured in the diamond anvil cell as a function of applied load. Results indicated serious difficulties in correlating pressure and applied load. A pronounced hysteresis was also observed.


1983 ◽  
Vol 22 ◽  
Author(s):  
G. J. Piermarini ◽  
R. G. Munro ◽  
S. Block

ABSTRACTThe pressure and temperature parameters which delineate the equilibrium thermodynamic stability fields of the liquid, VI and VII phases, includinq the triple point, were measured for the H2;0 and D2;0 systems over the pressure range, 0.8 to 2.4 GPa, and the temperature interval, 20 to 135 °C. The phenomenon of metastability associated with the liquid-VII phase boundary was observed during this work; and, subsequently, a metastable extension of this coexistence curve was determined from the liquid-VI-VII triple point down to 20 °C for both H2;0 and D2;0. The measurements were made by optical polarizing microscopy in conjunction with a diamond anvil cell equipped with a miniature resistance coil heatinq element. Pressures were measured by the ruby fluorescence method.


2008 ◽  
Vol 41 (2) ◽  
pp. 249-251 ◽  
Author(s):  
Stephen A. Moggach ◽  
David R. Allan ◽  
Simon Parsons ◽  
John E. Warren

A modification to the Merrill–Bassett miniature diamond anvil cell is reported here, with the inclusion of tungsten carbide backing seats with Boehler–Almax-cut diamonds to replace the previously used beryllium seats and (typically) modified brilliant-cut anvils. This has led to the removal of troublesome beryllium powder lines from diffraction images, while maintaining the pressure range and opening angle of the original design.


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