1989
DOI: 10.2320/matertrans1989.30.695
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Dynamical Behavior of Ordering with Phase Separation in Off-Stoichiometric Fe<SUB>3</SUB>Si Alloys

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Cited by 35 publications
(14 citation statements)
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“…The current study exhibits a qualitatively-similar phaseevolution pathway[15]. Liebscher et al suggested possible mechanisms on the formation of the hierarchical structure in the precipitates[32,[42][43][44], which involves a wetting transition or heterogeneous nucleation on L2 1 APBs[15,43,44]. The narrow anti-phase domain boundary formed within the L2 1 precipitate is believed to be responsible for the formation of the fine lamellar-type (hierarchical) structure for the 2% Ti alloy.…”
supporting
confidence: 60%
“…The current study exhibits a qualitatively-similar phaseevolution pathway[15]. Liebscher et al suggested possible mechanisms on the formation of the hierarchical structure in the precipitates[32,[42][43][44], which involves a wetting transition or heterogeneous nucleation on L2 1 APBs[15,43,44]. The narrow anti-phase domain boundary formed within the L2 1 precipitate is believed to be responsible for the formation of the fine lamellar-type (hierarchical) structure for the 2% Ti alloy.…”
supporting
confidence: 60%
“…The model 2 qualitatively corresponds to the Fe-Si-type alloys. The v n -values for this model were taken from the MFA calculations of Inden [31] which satisfactorily describe the relevant part of the observed Fe-Si phase diagram [4,32] with the following relations [33]:…”
Section: Models and Methods Of Simulationmentioning
confidence: 99%
“…Later stages correspond to the formation of more or less extended ordered regions which are more conveniently described by local order parameter distributions. Such distributions are experimentally observed in the diffraction transmission electron microscopy (TEM) images where the reflection intensity for a certain superstructure vector is proportional to the squared value of the relevant order parameter [1][2][3][4][5][6][7]. In particular, for the vector g 1 defined in equation 1the reflection intensity for the homogeneous D0 3 phase is proportional to η 2 and vanishes at η-APBs, while for the vector g 2 in equation 2this intensity for the homogeneous D0 3 phase is proportional to ζ 2 and vanishes both at ζ -APBs and η-APBs [6].…”
Section: A2mentioning
confidence: 99%
“…It occurs during decomposition of a homogeneous disordered phase into a two-phase mixture of ordered and disordered phases. Its dynamics has been explored recently by various techniques including computer simulations [1][2][3], thermodynamic stability analyses [4][5][6], and experiments [7][8][9][10]. However, the efifect of long-range Coulomb interaction on the nonlinear dynamics of ordering and phase separation seems to have never been discussed, although it is directly related to the interesting phenomenon of nanoscale ordered domain formation in oxide compounds, /^ (^1/3^2/3)03, where A, B\ and B" are cations with different valences.…”
mentioning
confidence: 99%