scholarly journals Unconventional phase III of high-pressure solid hydrogen

2019 ◽  
Vol 100 (15) ◽  
Author(s):  
Sam Azadi ◽  
Thomas D. Kühne
2017 ◽  
Vol 19 (32) ◽  
pp. 21829-21839 ◽  
Author(s):  
Sam Azadi ◽  
Graeme J. Ackland

Our study of the van der Waals interactions in solid molecular hydrogen structures indicates two candidates for phase III.


1997 ◽  
Vol 101-103 ◽  
pp. 1003-1005 ◽  
Author(s):  
B BARANOWSKI
Keyword(s):  

Author(s):  
Wai-Leung Yim ◽  
Hongliang Shi ◽  
Yunfeng Liang ◽  
Russell J. Hemley ◽  
John S. Tse

1988 ◽  
Vol 88 (1) ◽  
pp. 478-480 ◽  
Author(s):  
Joop van Straaten ◽  
Isaac F. Silvera

2016 ◽  
Vol 94 (13) ◽  
Author(s):  
Bartomeu Monserrat ◽  
Richard J. Needs ◽  
Eugene Gregoryanz ◽  
Chris J. Pickard

2020 ◽  
Vol 152 (7) ◽  
pp. 074701 ◽  
Author(s):  
Xingxing Jiang ◽  
Yueshao Zheng ◽  
Xiong-Xiong Xue ◽  
Jiayu Dai ◽  
Yexin Feng

2002 ◽  
Vol 14 (44) ◽  
pp. 10609-10613 ◽  
Author(s):  
Masaharu Takumi ◽  
Takeshi Masamitsu ◽  
Kiyofumi Nagata

2018 ◽  
Vol 112 (11) ◽  
pp. 111602 ◽  
Author(s):  
Haile Lei ◽  
Wei Lin ◽  
Kai Wang ◽  
Xibo Li

1981 ◽  
Vol 14 (6) ◽  
pp. 447-450 ◽  
Author(s):  
R. B. Roof

The structure of high-pressure americium, phase III, which occurs at room temperature in the pressure range 10–15 GPa, has been determined. The material has a monoclinic lattice with a = 3.025±0.005, b = 11.887±0.019, c = 2.830±0.005 Å, and β = 106.11±0.14° at 12.5 GPa. The space group is P21/m with Z = 4. Intensity data were obtained from powder-pattern films taken at pressure with Mo Kα radiation, λ = 0.7107 Å. The structure, which can be described as a layer stacking intermediate between the lower-pressure f.c.c. and higher-pressure α-U structure types, was refined by least-squares calculations to R 1 = 0.07 with 12 observed reflections. Am–Am distances of nearest neighbors range from 2.83 to 3.21 Å.


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