nonequilibrium growth
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2021 ◽  
Vol 7 (12) ◽  
pp. eabf2725
Author(s):  
Takayoshi Katase ◽  
Yudai Takahashi ◽  
Xinyi He ◽  
Terumasa Tadano ◽  
Keisuke Ide ◽  
...  

Material properties depend largely on the dimensionality of the crystal structures and the associated electronic structures. If the crystal-structure dimensionality can be switched reversibly in the same material, then a drastic property change may be controllable. Here, we propose a design route for a direct three-dimensional (3D) to 2D structural phase transition, demonstrating an example in (Pb1−xSnx)Se alloy system, where Pb2+ and Sn2+ have similar ns2 pseudo-closed shell configurations, but the former stabilizes the 3D rock-salt-type structure while the latter a 2D layered structure. However, this system has no direct phase boundary between these crystal structures under thermal equilibrium. We succeeded in inducing the direct 3D-2D structural phase transition in (Pb1−xSnx)Se alloy epitaxial films by using a nonequilibrium growth technique. Reversible giant electronic property change was attained at x ~ 0.5 originating in the abrupt band structure switch from gapless Dirac-like state to semiconducting state.


2018 ◽  
Vol 7 (3) ◽  
pp. 1801272 ◽  
Author(s):  
Mei Dong ◽  
Wei Zheng ◽  
Cunhua Xu ◽  
Richeng Lin ◽  
Dan Zhang ◽  
...  

2013 ◽  
Vol 203 (2) ◽  
pp. 359-372 ◽  
Author(s):  
Benedetta Cerruti ◽  
Alberto Puliafito ◽  
Annette M. Shewan ◽  
Wei Yu ◽  
Alexander N. Combes ◽  
...  

The growth of a well-formed epithelial structure is governed by mechanical constraints, cellular apico-basal polarity, and spatially controlled cell division. Here we compared the predictions of a mathematical model of epithelial growth with the morphological analysis of 3D epithelial structures. In both in vitro cyst models and in developing epithelial structures in vivo, epithelial growth could take place close to or far from mechanical equilibrium, and was determined by the hierarchy of time-scales of cell division, cell–cell rearrangements, and lumen dynamics. Equilibrium properties could be inferred by the analysis of cell–cell contact topologies, and the nonequilibrium phenotype was altered by inhibiting ROCK activity. The occurrence of an aberrant multilumen phenotype was linked to fast nonequilibrium growth, even when geometric control of cell division was correctly enforced. We predicted and verified experimentally that slowing down cell division partially rescued a multilumen phenotype induced by altered polarity. These results improve our understanding of the development of epithelial organs and, ultimately, of carcinogenesis.


2013 ◽  
Vol 87 (3) ◽  
Author(s):  
C. S. Dias ◽  
N. A. M. Araújo ◽  
M. M. Telo da Gama

2011 ◽  
Vol 6 (1) ◽  
pp. 477 ◽  
Author(s):  
Qian Li ◽  
Kui Cheng ◽  
Wenjian Weng ◽  
Chenlu Song ◽  
Piyi Du ◽  
...  

2011 ◽  
Vol 1297 ◽  
Author(s):  
D. J. Watts ◽  
D. D. Johnson ◽  
Daniel Finkenstadt

AbstractDensity-functional theory (DFT) calculations of interphase boundary energies provide useful input for many precipitate growth models in alloy systems [1]. One example is Al-Ag, where a rich variety of precipitate types exist, and the sizes and shapes are determined roughly by a Wulff construction, namely, minimizing surface free energies with respect to geometry. This is only a first approximation, however, as kinetic-considerations and crystallography do not allow for a uniform, isotropic growth. Consequently, a nonequilibrium growth model is developed for γ-plates [2], which attempts to connect semi-coherent (ledge) and incoherent (edge) interface growth rates in a way that incorporates shape and interface energies. Through this connection, we make a DFT model with approximate unit cells that mirror experimental conditions, which gives accurate predictions for precipitate aspect ratios and time-development of nonequilibrium shapes. Starting from an explicit calculation of Suzuki segregation of solute to stacking-faults, we find a mechanism for nucleation of nanoscale γ-plates on quenched defects, identify a bulk structure from a calculated phase diagram that gives the relevant HCP equilibrium precipitate structure occurring at 50 at.% Ag and calculate critical nucleation parameters for γ-precipitate formation. Applications to island-coarsening and lath morphology are also discussed.


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