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Numéro
J. Phys. II France
Volume 1, Numéro 7, July 1991
Page(s) 763 - 772
DOI https://doi.org/10.1051/jp2:1991108
References of J. Phys. II France 1 763-772
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  29. Fournier J B , Durand G , to be published
  30. All Bragg spots (${hk\ell}$) with ${h + k + \ell}$ odd are forbidden by the bcc symmetry , in particular, this means that the effective spacing between dense planes along a $\langle111\rangle$ direction is $a/2 \sqrt{3}$ (i e 34 Å) instead of $a/ \sqrt{3},$ and $a/2 \sqrt{5}$ (i.e 26 4 Å) instead of $a/ \sqrt{5}$ along a $\langle210\rangle$ direction
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  33. Intersections of a facet with the planes of non-adjacent facets would correspond to other lines in its plane In this case, the angles between intersecting planes are larger, closer to 90$^{\circ}$ The extra energy associated with edges (or furrows) may be higher in that case
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  36. There remains also a contribution from edges (or furrows), which should be comparable to the energy associated to $\ll$ unit $\gg$ dislocation cores