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2
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0000595740
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H. Kobayashi, M. Sato, T. Kamimura, M. Sakai, H. Onodera, N. Kuroda, and Y. Yamaguchi, J. Phys.: Condens. Matter 9, 515 (1997).
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Kobayashi, H.1
Sato, M.2
Kamimura, T.3
Sakai, M.4
Onodera, H.5
Kuroda, N.6
Yamaguchi, Y.7
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11
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0028811712
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Y. Fei, C. T. Prewitt, H. K. Mao, and C. M. Bertka, Science 268, 1892 (1995).
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Science
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Fei, Y.1
Prewitt, C.T.2
Mao, H.K.3
Bertka, C.M.4
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12
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0031075284
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K. Kusaba, Y. Syono, T. Kikegawa, and O. Shimomura, J. Phys. Chem. Solids 58, 241 (1997).
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J. Phys. Chem. Solids
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Kusaba, K.1
Syono, Y.2
Kikegawa, T.3
Shimomura, O.4
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13
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85024722413
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R. J. Nelmes, M. I. McMahon, S. A. Belmonte, D. R. Allan, M. R. Gibbs, and J. B. Parise, Rev. High Pressure Sci. Technol. 7, 202 (1998).
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Nelmes, R.J.1
McMahon, M.I.2
Belmonte, S.A.3
Allan, D.R.4
Gibbs, M.R.5
Parise, J.B.6
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16
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85037897299
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The reflection indexed as (302) by Kusaba et al. (Ref. 12) is clearly indexed correctly as (013) in our patterns.
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The reflection indexed as (302) by Kusaba et al. (Ref. 12) is clearly indexed correctly as (013) in our patterns.
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17
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85037906081
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Kusaba et al. (Ref. 12) propose that the monoclinic shear is in the basal plane, but that is inconsistent both with the space-group symmetry—for a NiAs-like structure—and also with a strong contraction along the NiAs C axis.
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Kusaba et al. (Ref. 12) propose that the monoclinic shear is in the basal plane, but that is inconsistent both with the space-group symmetry—for a NiAs-like structure—and also with a strong contraction along the NiAs C axis.
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18
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85037915971
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The a-glide relates atoms (Formula presented) apart in the FeS-III structure, and this corresponds to atoms related by the a-glide operation plus a lattice repeat along (Formula presented) in the MnP structure, i.e., (Formula presented)
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The a-glide relates atoms (Formula presented) apart in the FeS-III structure, and this corresponds to atoms related by the a-glide operation plus a lattice repeat along (Formula presented) in the MnP structure, i.e., (Formula presented)
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-
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20
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85037906622
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Refinement of a mixed-phase pattern at 7.1 GPa gives (Formula presented) (Formula presented) (Formula presented) for the MnP phase, and (Formula presented) (Formula presented) (Formula presented) (Formula presented) for the FeS-III phase. The volume difference of 6.7(2)% is smaller than found in Ref. 8, but agrees with Ref. 12
-
Refinement of a mixed-phase pattern at 7.1 GPa gives (Formula presented) (Formula presented) (Formula presented) for the MnP phase, and (Formula presented) (Formula presented) (Formula presented) (Formula presented) for the FeS-III phase. The volume difference of 6.7(2)% is smaller than found in Ref. 8, but agrees with Ref. 12.
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21
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0030515880
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N. G. Wright, R. J. Nelmes, S. A. Belmonte, and M. I. McMahon, J. Synchrotron Radiat. 3, 112 (1996).
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(1996)
J. Synchrotron Radiat.
, vol.3
, pp. 112
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Wright, N.G.1
Nelmes, R.J.2
Belmonte, S.A.3
McMahon, M.I.4
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