Authors: Rositza Yakimova, Gholam Reza Yazdi, Nut Sritirawisarn, Mikael Syväjärvi
Abstract: We report on growth of 3C-SiC by sublimation process in vacuum with the aim to
ultimately select conditions for single polytype growth of bulk crystals. The 3C polytype
occurrence, growth mechanism and structure evolution have been in the focus of the study. To gain
understanding of the initial formation of the cubic polytype, growth was performed on various
substrates, such as 6H- and 4H-SiC (on-axis and vicinal), as well as freestanding 3C-SiC wafers.
The growth configuration used allowed a high growth rate, e.g. up to 200 (m/h, respectively very
thick layers. The grown material was studied by means of optical microscopy, AFM and HRTEM.
6H-SiC (0001) Si-face substrates may be a good choice if the 3C nucleation is well controlled,
which can be achieved by selecting the initial temperature ramp up and substrate orientation. These
growth conditions limit the number of nucleation centers and decrease the defective boundaries.
283
Authors: Guido Schmitz, Constantin Ene, Ch. Lang, Vitaliy Vovk
Abstract: Down-scaling is a major principle of modern technology. As a consequence, the
stability of many technical devices is controlled by solid state reactions that proceed on the range of
a few nanometres only. On such a short length scale even basic aspects of reaction physics as
fundamental as e.g. the Ficks laws of diffusion, need to be reconsidered.
Only very few dedicated techniques are suitable to study atomic transport and reactions with
sufficient accuracy. Among them, the atom probe tomography is exceptional, as it allows the
detection and localization of individual atoms with an accuracy of a lattice constant. An almost
complete reconstruction of the 3D atomic arrangement of different atomic species gets possible.
This article provides an overview on recent atom probe studies of reactive diffusion. After an
introduction into the principles of the analysis method, physical mechanisms of solid state reactions
are discussed in view of recent experiments at metallic thin film interfaces. How does nucleation of
an interfacial product take place In which way do grain boundaries influence the reaction As a
technical example, the stability of Cu/NiFe GMR sensor layers is discussed.
126
Authors: Robert L. Karlinsey, Anderson T. Hara, Clif W. Duhn
Abstract: Self-assembled niobium oxide microcones produced by potentiostatic anodization with varied
NaF content (between 100 and 250 mg) in an HF electrolyte are shown to nucleate mineral when
immersed in supersaturated solutions emulating mineral content in saliva and blood. The most
extensive mineral coverage in 100 mL of 2.5 wt. % HF electrolyte occurs when NaF content is
about 100 mg with substantial mineral formation occurring within 24 hours. Higher salt content
apparently alters the conditions favoring mineral nucleation by generating smaller nucleation
centers that ultimately diminish the extent of mineral coverage. Additionally, nucleation kinetics
and morphological contrasts between mineral formed from saliva and blood is briefly discussed in
terms of the relative degree of supersaturation with respect to hydroxyapatite. Finally, we show that
the integrity of the microcone shape is not critical for mineral nucleation, an observation that builds
on our prior hypothesis by promoting the importance of self-assembly and crystal formation. Based
on these results, we demonstrate the influence of NaF and stress the role of the self-organization
process in producing effective mineral nucleation sites.
17
Authors: Michael Hitchcock, Zhong Yun Fan
Abstract: Solidification behaviour of 357 Al-alloy under intensive forced convection in the rheo-die-casting
(RDC) process, was investigated experimentally to understand the effects of the intensity of forced
convection and shearing time on the nucleation and growth behaviour. It was found that under
intensive forced convection, heterogeneous nucleation occurred continuously throughout the entire
volume of the solidifying melt. All the nuclei could survive due to the uniform temperature and
composition fields created by the forced convection. This has been named as ‘effective and
continuous nucleation’. It is also found that the nuclei grow spherically with an extremely fast
growth rate. This makes the primary solidification essentially a slow coarsening process, in which
Ostwald ripening takes place by dissolution of the smaller particles. In addition, it was found that
intensive forced convection suppresses partially the formation of the primary phase, promote
nucleation of the primary particles, and hinders the particle growth.
1747
Authors: Shang Ping Chen, A. Miroux, Sybrand van der Zwaag
Abstract: A simple model for recovery of a subgrain structure is used to distinguish and explain the
respective influence of the deformed microstructure characteristics, annealing temperature and
concurrent precipitation kinetics on the nucleation kinetics of recrystallisation. Simulation results
demonstrate how the balance between recovery and precipitation kinetics controls nucleation.
1605
Authors: Katsura Kajihara, Kazuhide Matsumoto, Katsushi Matsumoto
Abstract: This study presents in situ observations of recrystallization texture formation in
Al-3mass%Mg using SEM concurrent with electron back scattering pattern (EBSP) with hot stage. In
the present discussion, the emphasis is on the characteristics of the preferred growth or the shrinkage
of Cube and other oriented grains. The in-situ observations of recrystallization demonstrate clearly
that the nucleation, growth and shrinkage of recrystallized grains occur simultaneously in each
orientation in each region. The overall development of recrystallization texture depends on the
balance of nucleation/growth and shrinkage/disappearance of each orientation during
recrystallization. The preferential growth is determined by the grain boundary mobility between
recrystallized grains or the clusters composed of several similar oriented grains, i.e. Cube clusters or S
clusters, and neighboring deformed matrix, and the competitive growth with the surrounding grains.
On the other hand, the isolated oriented grain and the strain-stored grains tend to shrink and disappear
during recrystallization and grain growth.
1579
Authors: Dorte Juul Jensen
Abstract: By 3 dimensional X-ray diffraction (3DXRD) using high energy X-rays from
synchrotron sources it is possible to study in-situ the nucleation and growth during recrystallization.
In this paper it is described and discussed how 3DXRD can supplement EBSP measurements of
nucleation and growth. Three types of studies are considered: i) orientation relationships between
nuclei and parent deformed matrix, ii) recrystallization kinetics of individual bulk grains and iii)
filming of growing grains in deformed single crystals.
1569
Authors: Christophe Sigli
Abstract: A kinetic model has been developed to simulate the precipitate size distribution and the
resulting yield strength during ageing of 7xxx alloys. The η phase is the only one considered. The
kinetic model is mean field: precipitates of different sizes see each other through the average solid
solution. Precipitates are assumed to be homogeneous in concentration and are allowed to change
chemistry. Local equilibrium is assumed at the matrix-precipitate interface; the equilibrium
concentrations are corrected by the curvature effect. Values of the equilibrium concentrations at the
matrix-precipitate interface are solved by an iterative method: the resulting flux for each element
must be compatible with equilibrium conditions and with the changing stoechiometry of the
considered precipitate while maximizing the energy gained. The yield strength is derived from the
precipitate size distribution through a mixture law combining the effect of each individual
precipitate. The model can take into account non-isothermal treatments and can therefore simulate
complicated multi-stage ageing treatment as well as a FSW weld. Results of the model are discussed
and compared measurements.
321
Authors: S. Esmaeili, David J. Lloyd
Abstract: The role of Cu in precipitation behavior of 6000 series aluminum alloys has been investigated by
isothermal calorimetry and transmission electron microscopy. The newly developed analytical
techniques have been used to evaluate the precipitation kinetics in alloys with or without an initial
pre-aging history. It has been found that Cu addition results in increasing the rate of precipitation
when artificial aging is applied immediately after solutionizing and quenching. However, Cu has no
significant effect on the kinetics of precipitation in alloys with the pre-aging history, while it
produces finer microstructures in the pre-aged and then artificially aged alloys. These observations
have been explained by the effect of Cu on increasing the rate of precipitate nucleation in 6000
series alloys. It has also been suggested that the effect of Cu on nucleation arises from the role of
Cu on the cluster formation during and/or immediately after quenching.
169
Authors: Karl Martin Pedersen, Niels Tiedje
Abstract: Hypereutectic ductile iron was cast in green sand moulds with four plates with thickness of 1.5, 2, 3 and 4 mm in each mould. Temperatures were measured in the 3 and 4 mm plate. The temperature curves showed that eutectic solidification was divided into two stages: primary and secondary eutectic solidification. The first stage, which was relatively short, had none or very little recalescence. Further under cooling, followed by reheating during recalescence, was necessary to
initiate the second part of the eutectic solidification. Both the secondary under cooling and recalescence was larger in the 3 mm plates than in the 4 mm plates. All 1.5 mm plates contained carbides but the other plates solidified without carbides. Metallographic examination showed two populations of graphite nodules. A small group of nodules was larger than rest of the nodules. Color etching revealing the segregation of Si showed a higher Si content in the ferrite around the larger
nodules compared to the ferrite around the rest of the nodules. This indicates that solidification took place along the following path: The solidification starts with nucleation and growth of primary graphite nodules. This probably starts during the filling of the mould. The primary nodules act as nuclei for austenite. As austenite easily nucleates on graphite the temperature will be the same for the 3 and 4 mm plate for the first part of the eutectic solidification. This first part of the
solidification ends when concentration of carbon around austenite dendrites is too large and new nodules have to nucleate and grow. The larger under cooling for the 3 mm plates compared to the 4 mm indicates that the nucleation of new nodules is governed by kinetics even in very well inoculated melts.
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