Understanding the crystal structure of solid hydrogen under ultrahigh pressure

Scilight ◽  
2020 ◽  
Vol 2020 (43) ◽  
pp. 431105
Author(s):  
Aili McConnon
1966 ◽  
Vol 45 (3) ◽  
pp. 834-837 ◽  
Author(s):  
Charles S. Barrett ◽  
Lothar Meyer ◽  
Judith Wasserman

Nature ◽  
1967 ◽  
Vol 213 (5072) ◽  
pp. 171-172 ◽  
Author(s):  
E. SÁNDOR ◽  
R. F. C. FARROW

2020 ◽  
Vol 105 (9) ◽  
pp. 1432-1435
Author(s):  
Luca Bindi ◽  
Mark D. Welch ◽  
Aleksandra A. Bendeliani ◽  
Andrey V. Bobrov

Abstract The crystal structure of a new high-pressure hydrous phase, Si-rich Mg-sursassite, of ideal composition Mg4Al5Si7O23(OH)5, that was produced by sub-solidus reaction at 24 GPa and 1400 °C in an experiment using a model sedimentary bulk composition, has been determined by single-crystal X-ray diffraction. The phase was found to be topologically identical to Mg-sursassite, Mg5Al5Si6O21(OH)7, and has space group P21/m and lattice parameters a = 8.4222(7), b = 5.5812(3), c = 9.4055(9) Å, b = 106.793(8)°, V = 423.26(6) Å3, and Z = 1. The empirical formula determined by electron microprobe analysis of the same crystal as was used in the X-ray experiment is [Mg3.93(3)Fe0.03(1)]Σ3.96[Al4.98(3)Cr0.04(1)]S5.02 Si7.02(4)O23(OH)5, with hydroxyl content implied by the crystal-structure analysis. The most significant aspect of the structure of Si-rich Mg-sursassite is the presence of octahedrally coordinated Si. Its structural formula is M1,VIIMg2M2,VIMg22+M3,VI(Al0.5Si0.5)2M4,VIAl2M5,VIAl2T1,IVSi2T2,IVSi2T3,IVSi2 O23(OH)5. Si-rich Mg-sursassite joins the group of hydrous ultrahigh-pressure phases with octahedrally coordinated Si that have been discovered by experiment, and that may play a significant role in the distribution and hosting of water in the deep mantle at subduction zones. The reactions defining the stability of Si-rich Mg-sursassite are unknown, but are likely to be fundamentally different from those of Mg-sursassite, and involve other ultrahigh-pressure dense structures such as phase D, rather than phase A.


1962 ◽  
Vol 1 (1) ◽  
pp. 22-23 ◽  
Author(s):  
J. Van Kranendonk ◽  
H.P. Gush

1972 ◽  
Vol 50 (18) ◽  
pp. 2063-2073 ◽  
Author(s):  
S. A. Boggs ◽  
M. J. Clouter ◽  
H. L. Welsh

Spectra of the infrared fundamental band of solid hydrogen with orthohydrogen concentrations in the range 75 to ~99% were recorded at 1.05 and ~5 K, i.e. below and above the order–disorder phase transition which occurs at 2.8 K for pure o-H2. The effect of "impurity" para molecules in the o-H2 lattice could thus be studied with and without orientational ordering of the o-H2 molecules. The zero-phonon Q1, S1(0), and S1(1) features are of particular interest, and are interpreted in terms of travelling vibrational, rotational, and orientational excitations (vibrons, rotons, and librons). The Q branch for ~100% o-H2 in the ordered state shows a structured side band, shifted by ~6–26 cm−1 from the Q1(1) frequency and due to one- and two-libron excitations; in the disordered state this becomes a Boltzmann-modified band of half-width 12 cm−1, centered at the Q1(1) frequency, and due to predominantly low-energy orientational transitions of interacting o-H2 molecules. The S1(0) group of maxima in the ordered state is interpreted as the superposition of the transitions, Q1(1) + S0(0) and Q1(1) + S0(0) + libron, where Q1(1) is an o-H2 vibron and S0(0) is the localized rotational transition of an impurity p-H2 molecule, the J = 2 level of which is split into three sublevels by the C3i field of the Pa3 crystal structure.


1998 ◽  
Vol 57 (10) ◽  
pp. 5699-5703 ◽  
Author(s):  
S. Endo ◽  
A. Honda ◽  
K. Koto ◽  
O. Shimomura ◽  
T. Kikegawa ◽  
...  

2020 ◽  
Vol 5 (3) ◽  
pp. 038401 ◽  
Author(s):  
Cheng Ji ◽  
Bing Li ◽  
Wenjun Liu ◽  
Jesse S. Smith ◽  
Alexander Björling ◽  
...  

2016 ◽  
Vol 101 (2) ◽  
pp. 355-361 ◽  
Author(s):  
Aaron Lussier ◽  
Neil A. Ball ◽  
Frank C. Hawthorne ◽  
Darrell J. Henry ◽  
Rentaro Shimizu ◽  
...  

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