2001
DOI: 10.1016/s1359-6454(01)00155-0
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On the origin of the high coarsening resistance of Ω plates in Al–Cu–Mg–Ag Alloys

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Cited by 234 publications
(147 citation statements)
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“…The angle between the normal of the boundary plane and the normal of the Ω-phase platelets ranges from 0 to 451 to fit the orientation of this phase to a {111} α habit plane. Only one broad interface of a thick Ω-phase retains fully coherent configuration and specific OR [1,[3][4][5]8,12,14], while the opposite broad interface has a fully or partially semi-coherent structure, and OR at this interface deviate from the (001) Ω //(111) α on the value of misorientation (Z41) of a deformation-induced boundary (Fig. 16).…”
Section: Precipitation Behavior During Agingmentioning
confidence: 99%
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“…The angle between the normal of the boundary plane and the normal of the Ω-phase platelets ranges from 0 to 451 to fit the orientation of this phase to a {111} α habit plane. Only one broad interface of a thick Ω-phase retains fully coherent configuration and specific OR [1,[3][4][5]8,12,14], while the opposite broad interface has a fully or partially semi-coherent structure, and OR at this interface deviate from the (001) Ω //(111) α on the value of misorientation (Z41) of a deformation-induced boundary (Fig. 16).…”
Section: Precipitation Behavior During Agingmentioning
confidence: 99%
“…16). This deviation is attributed to the high density of the thickening ledge [4,8,17,25] on the semi-coherent board interfaces. Therefore, the deformation banding leads to the appearance of relatively coarse platelets of the Ω-phase along the {111} α plane with a semi-coherent interface due to heterogeneous nucleation and accelerated growth at dislocation boundaries or boundaries of shear bands.…”
Section: Precipitation Behavior During Agingmentioning
confidence: 99%
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