The structural features and energetics of Znn−mCdm (n=7,8) microclusters and Zn50, Cd50, and Zn25Cd25 nanoparticles have been investigated by performing molecular-dynamics computer simulations using a recently developed empirical many-body potential-energy function. The most stable structures were found to be compact and three-dimensional for all elemental and mixed clusters. An interesting structural feature of the mixed clusters is that Zn and Cd atoms do not mix in mixed clusters; they come together almost without mixing
Surface and core formation, thermal and electronic properties of ternary cubic CdZnTe clusters are i...
Gold nanoclusters in the size range of 3-8 nm in diameter (923-10179) atoms were studied using the e...
(MgO)60 and (ZnO)60 are predicted to be magic-number clusters in the shapes of cuboid (CB) and doubl...
An empirical many-body potential energy function has been developed to investigate the structural fe...
Using an empirical potential energy function parametrized for each of the Ni, Cu, Pd, Pt, and Pb sys...
The structural and electronic properties of isolated neutral ZnmCdn clusters for m + n less than or ...
We have investigated the energetics and the structural stability of gold microclusters containing 3–...
The Gupta-type many-body potential was applied to describe the interactions between atoms in zinc na...
Structural stability and energetics of zirconium microclusters Zr, (n = 3-13) have been investigated...
Structural stability and energetics of uranium microclusters, U-n (n = 3-13, 27-137), have been inve...
We have investigated the energetics and the structural stability of gallium microclusters including ...
Static average polarizabilities, alpha, and second hyperpolarizabilities, gamma, of ZnmCdn nanoclust...
Structural properties of zinc oxide (ZnO) nanoparticles and nanorings have been investigated by perf...
A recently developed empirical many-body potential energy function (PEF) has been modified and param...
Platinum-cobalt bimetallic clusters (N = 11-15) were modeled by a many-body Sutton-Chen (SC) potenti...
Surface and core formation, thermal and electronic properties of ternary cubic CdZnTe clusters are i...
Gold nanoclusters in the size range of 3-8 nm in diameter (923-10179) atoms were studied using the e...
(MgO)60 and (ZnO)60 are predicted to be magic-number clusters in the shapes of cuboid (CB) and doubl...
An empirical many-body potential energy function has been developed to investigate the structural fe...
Using an empirical potential energy function parametrized for each of the Ni, Cu, Pd, Pt, and Pb sys...
The structural and electronic properties of isolated neutral ZnmCdn clusters for m + n less than or ...
We have investigated the energetics and the structural stability of gold microclusters containing 3–...
The Gupta-type many-body potential was applied to describe the interactions between atoms in zinc na...
Structural stability and energetics of zirconium microclusters Zr, (n = 3-13) have been investigated...
Structural stability and energetics of uranium microclusters, U-n (n = 3-13, 27-137), have been inve...
We have investigated the energetics and the structural stability of gallium microclusters including ...
Static average polarizabilities, alpha, and second hyperpolarizabilities, gamma, of ZnmCdn nanoclust...
Structural properties of zinc oxide (ZnO) nanoparticles and nanorings have been investigated by perf...
A recently developed empirical many-body potential energy function (PEF) has been modified and param...
Platinum-cobalt bimetallic clusters (N = 11-15) were modeled by a many-body Sutton-Chen (SC) potenti...
Surface and core formation, thermal and electronic properties of ternary cubic CdZnTe clusters are i...
Gold nanoclusters in the size range of 3-8 nm in diameter (923-10179) atoms were studied using the e...
(MgO)60 and (ZnO)60 are predicted to be magic-number clusters in the shapes of cuboid (CB) and doubl...