1996
DOI: 10.1007/bf02651872
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The role of coincident site lattice boundaries during selective growth in interstitial-free steels

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Cited by 7 publications
(3 citation statements)
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“…The particular nuclei exhibiting CSL boundaries will not inherit their orientation from the deformed neighboring grains (termed as orientation selectivity) [ 23 ], which would be beneficial to add more variety in terms of orientation other than the orientation of the deformed grains. In addition, CSL boundaries with rotation axes parallel to especially the axis and axis were favorable for the growth of nuclei [ 24 , 25 ]. Moreover, in the case of Σ7, the growth was expected to be rapid and contributed significantly to final recrystallization textures via the selective growth mechanism [ 26 ].…”
Section: Resultsmentioning
confidence: 99%
“…The particular nuclei exhibiting CSL boundaries will not inherit their orientation from the deformed neighboring grains (termed as orientation selectivity) [ 23 ], which would be beneficial to add more variety in terms of orientation other than the orientation of the deformed grains. In addition, CSL boundaries with rotation axes parallel to especially the axis and axis were favorable for the growth of nuclei [ 24 , 25 ]. Moreover, in the case of Σ7, the growth was expected to be rapid and contributed significantly to final recrystallization textures via the selective growth mechanism [ 26 ].…”
Section: Resultsmentioning
confidence: 99%
“…While oriented nucleation dominates the formation of many recrystallization textures [1][2][3][4][5], some are substantially modified by selective growth [2,[6][7][8]. Experiments have shown that boundaries with certain misorientations, such as 27°<110> in Fe-Si [9,10] and 40°<111> in Al [11,12] are more mobile than other boundaries, giving rise to selective growth.…”
Section: Introductionmentioning
confidence: 99%
“…It is comparable to textures reported in the literature for cold-rolled IF steels of relatively similar composition and rolling reduction. 13,24,25) The density along the RDfibre increases steadily from 6 at Fϭ0°, ͕001͖͗110͘, to a peak of 10 at Fϭ30°, half-way between ͕113͖͗110͘ and ͕112͖͗110͘. Beyond Fϭ45°, the density decreases rapidly, dropping below 1 at Fϭ70°.…”
mentioning
confidence: 99%