1993
DOI: 10.1016/0022-3093(93)90304-g
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Neutron scattering structural study of AlCuFe quasicrystals using double isotopic substitution

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Cited by 25 publications
(5 citation statements)
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“…This brings up a question: are partial amplitudes a k experimentally measurable? Since formally a k can be derived (up to a common phase factor) through the dependence of the Bragg peak intensities (20) on the weights w p , one can think of using the method of isotopic substitution in neutron diffraction experiments [24]. However, this approach does not allow to distinguish the contributions of the same chemical element in different local environments.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…This brings up a question: are partial amplitudes a k experimentally measurable? Since formally a k can be derived (up to a common phase factor) through the dependence of the Bragg peak intensities (20) on the weights w p , one can think of using the method of isotopic substitution in neutron diffraction experiments [24]. However, this approach does not allow to distinguish the contributions of the same chemical element in different local environments.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…This brings up a question: are partial amplitudes a k experimentally measurable? Since formally a k can be derived (up to a common phase factor) through the dependence of the Bragg peak intensities (20) on the weights w p , one can think of using the method of isotopic substitution in neutron diffraction experiments [21]. However, this approach does not allow to distinguish the contributions of the same chemical element in different local environments.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…A 3D model of the AlCuFe icosahedral structure has been obtained by irrational projection in parallel space (3D real space) of the nodes of a 6D hypercubic lattice [3,4,9]. It was determined from a 6D neutron diffraction study [10] that the AlCuFe icosahedral structure is defined in 6D space by 3 atomic surfaces located at the N [000000] and N [100000] nodes of a primitive lattice and at the BC 1/2[111111] body-centre; the other BC 1/2[111111] body-centre is vacant. The size and shape of the atomic surfaces, in perpendicular space, determine the occupation in real space of the nodes of the four sublattices: Figure 3 is a two-fold section of this 3D model, previously described by Le Lann and Devaud [5].…”
Section: Translation Defectsmentioning
confidence: 99%