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This trend is similar to that of scattering by a sphere, i.e., Mie scattering [23].
We also find that when the nodes are mapped to the bottom half sphere (i.e., ), CSR has the best performance compared with other sizes of the sphere.
The potential defined in Equation 2 confines the exciton in the upper half of a sphere, i.e., the quantum dot has a semi-spherical shape.
where the parameter y is a nonnegative point of the unit sphere, i.e., y ∈ Y = { y ∈ R l ∣ y ≥ 0, ∥ y ∥ = 1 }.
Assume that the furthest wireless node is of distance from the center (i.e., south pole of the sphere), then the value of the highest projection on the sphere (i.e., the value of ) is (2).
Extensive exploration of natural resources and adaptation to the environmental conditions gave rise to the relevant processes in the spiritual sphere, i.e., attached sacred signifi cance to specifi c landscape features.
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Two non convex bodies built from two spheres, i.e. dumbbells and diabolos, were considered.
The bed was made using two rows of spheres fixed in staggered positions, and a test sphere resting on top of the three neighbouring fixed spheres (i.e. nestling in the space between the surfaces of the fixed spheres).
When the average distance between spheres was reduced due to compression, surface pressure increased rapidly as a result of the strong interaction between spheres, i.e. adding a monolayer to the surface reduces the surface tension (γ < γ0).
As has been found in experiments, the so-called "normal" spheres, i.e., formed by the minority blocks, tend to pack into the bcc array, while the "inverted" spheres formed by the majority blocks favor the fcc packing.
Two of the oldest known classical integrable systems are: (i) n-decoupled harmonic oscillators, constrained to the surface of the n-sphere (i.e., the classical C. Neumann system), and (ii) geodesic flow on an n-axial ellipsoid.
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