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Techniques for neutron diffraction on solidified gases to 10 GPa and above: Applications to ND3 phase IV
1.For a review see, for example, Simple Molecular Systems at Very High Density, edited by A. Polian, P. Loubeyre, and N. Boccara (Plenum, New York, 1989).
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4.R. J. Nelmes, J. S. Loveday, R. M. Wilson, W. G. Marshall, J. M. Besson, S. Klotz, G. Hamel, T. Aselage, and S. Hull, Phys. Rev. Lett. 74, 2268 (1995).
5.R. J. Nelmes, J. S. Loveday, R. M. Wilson, J. M. Besson, Ph. Pruzan, S. Klotz, G. Hamel, and S. Hull, Phys. Rev. Lett. 71, 1192 (1993).
6.R. L. Mills (unpublished).
7.J. W. Otto, R. F. Porter, and A. L. Ruoff, J. Phys. Chem. Solids 50, 171 (1989).
8.R. J. Nelmes, J. S. Loveday, R. M. Wilson, J. M. Besson, S. Klotz, G. Hamel, and S. Hull, Trans. Am. Crystallogr. Assoc. 29, 19 (1993).
9.Although the crystal structure determination of phase IV in Ref. 7 is incorrect, the peaks that were used to evaluate the equation-of-state in a hexagonal setting (i.e., 100, 002, 101, 102, and 110) can be utilized as a pressure gauge, since they have been measured in Ref. 7 against the luminescence of ruby. The accuracy of the pressure values obtained in this way depends upon the accuracy of the equation-of-state and should be <±0.3 GPa.
10.The remaining space groups are: P222 (16), Pmm2 (25), Pmmm (47), (17), (18), (19), (26), P2cm (28), Pmcm (51), P2cb (32), and Pmcb (55).
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