1989
DOI: 10.1007/bf00898530
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Nucleation centers and wave schemes of martensite growth in iron alloys

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Cited by 6 publications
(3 citation statements)
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“…Then the overcoming of a finite energy barrier will be promoted by the longitudinal displacement mode with wavelength λ 3 = 2λ 1 synchronized with the transverse mode. In our opinion, this is a dominant mechanism in the plane shuffle, resulting in the final sequence A α B α A α B α A α B α … Note that the existence of breather-type excitations with synchronized transverse and longitudinal displacements, which are responsible for the change of the plane positioning sequence, was suggested earlier (without concrete definition of wavelength values) [13].…”
Section: Short-wave Displacements Changing the Plane Positioning Sequmentioning
confidence: 62%
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“…Then the overcoming of a finite energy barrier will be promoted by the longitudinal displacement mode with wavelength λ 3 = 2λ 1 synchronized with the transverse mode. In our opinion, this is a dominant mechanism in the plane shuffle, resulting in the final sequence A α B α A α B α A α B α … Note that the existence of breather-type excitations with synchronized transverse and longitudinal displacements, which are responsible for the change of the plane positioning sequence, was suggested earlier (without concrete definition of wavelength values) [13].…”
Section: Short-wave Displacements Changing the Plane Positioning Sequmentioning
confidence: 62%
“…This seems to be a reason for the predetermination of the selection of DNC's with <110> γ and <112> γ lines that correspond to the DWP [1-3]. However, having produced a selected system of dislocations with lines Λ along one of the <111> γ directions for as-quenched martensite, one can obtain a strongly pronounced orientation effect: the occurrence of crystals with habituses of type (13) which are collinear with Λ and have no more than six orientations. For strain-induced martensite, the orientation effect can be enhanced by stretching austenite along the selected <111> γ direction .…”
Section: Expected Habituses and Dislocation Nucleation Centers For Asmentioning
confidence: 99%
“…From Eq. (14) it follows that at θ = −π/2, the eigenvectors of the strain tensor are at angles of ±π/4 to the extra plane. This means that the extra plane for normals (9) coincides with the orientation of the habit plane.…”
mentioning
confidence: 98%