The energetic stability of coherent interfaces in core-shell binary nanocrystals is studied by atomistic modeling. Universal trends in preferential facet orientations are found, depending on the sign of the lattice mismatch between the elements. The results are explained in terms of structural relaxation processes common to all systems analyzed. These findings have a general character, so that they can be useful to understand and predict equilibrium shapes of small inclusions in systems where the Wulff theorem fails due to non-negligible strain. © 2014 American Physical Society
We study numerically the equilibrium shapes, shape transitions, and dislocation nucleation of small ...
A nearest neighbor, broken bond model is employed to develop general relationships for the concentra...
The reorganisation of nanocrystals in order to reduce their surface energies has been examined in co...
In this work, using the Cu–Ni (111) semi-coherent interface as a model system, we combine atomistic ...
The equilibrium structure of embedded nanocrystals formed from strongly segregating binary- alloys ...
We discuss the stability and free energy of 1D (chains), 2D (planar superlattices), and 3D (bcc or f...
Nanolayered metallic composites exhibit unusual high strength at the layer thickness in nanometers. ...
The energy density of crystal interfaces exhibits a characteristic “cusp” structure that renders it ...
The instability of nanocrystalline materials against both grain growth and bulk phase separation is ...
We present a detailed investigation of nanoparticle binary superlattices. We characterize the proper...
Understanding interfacial energy between crystal lattices is of great interest in modeling mechanica...
Several crystalline structures are metastable or kinetically frozen out-of-equilibrium states in the...
We develop an explicit model for the interfacial energy in crystals that emphasizes the geometric or...
International audienceIn this paper we establish a generalized Wulf-Kaishew theorem giving the equil...
In nanocrystalline alloys, a range of configurations c an have low energies when solute atoms have ...
We study numerically the equilibrium shapes, shape transitions, and dislocation nucleation of small ...
A nearest neighbor, broken bond model is employed to develop general relationships for the concentra...
The reorganisation of nanocrystals in order to reduce their surface energies has been examined in co...
In this work, using the Cu–Ni (111) semi-coherent interface as a model system, we combine atomistic ...
The equilibrium structure of embedded nanocrystals formed from strongly segregating binary- alloys ...
We discuss the stability and free energy of 1D (chains), 2D (planar superlattices), and 3D (bcc or f...
Nanolayered metallic composites exhibit unusual high strength at the layer thickness in nanometers. ...
The energy density of crystal interfaces exhibits a characteristic “cusp” structure that renders it ...
The instability of nanocrystalline materials against both grain growth and bulk phase separation is ...
We present a detailed investigation of nanoparticle binary superlattices. We characterize the proper...
Understanding interfacial energy between crystal lattices is of great interest in modeling mechanica...
Several crystalline structures are metastable or kinetically frozen out-of-equilibrium states in the...
We develop an explicit model for the interfacial energy in crystals that emphasizes the geometric or...
International audienceIn this paper we establish a generalized Wulf-Kaishew theorem giving the equil...
In nanocrystalline alloys, a range of configurations c an have low energies when solute atoms have ...
We study numerically the equilibrium shapes, shape transitions, and dislocation nucleation of small ...
A nearest neighbor, broken bond model is employed to develop general relationships for the concentra...
The reorganisation of nanocrystals in order to reduce their surface energies has been examined in co...