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In each ray of light.
It is similarly supported; a series of ambulacral ossicles in each ray roughly corresponds with the vertebrae of vertebrates.
The rays are disjoint with the exception of a single common point, and in each ray at most one potential target may be located.
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Furthermore, it allows for these checks to be performed in parallel and in advance for each ray.
In the first step, each ray in E i -1 is tested to determine whether it belongs to the hyperplane S i v = 0. Rays in E(K i - 1) that belong to this hyperplane are added to the collection E(K i ).
The mercury reflected light rays back through the emulsion to interfere with the incident rays, forming a latent image that varied in depth according to each ray's colour.
In such a diagram each ray (or point specifying a ray) is represented by a vertex.
The starting phases Φi,r are determined randomly between 0 and 2Π for each ray in every cluster.
In the second step of iteration i, the algorithm considers each ray pair in E(K i - 1) that lies on opposite sides of the hyperplane S i v = 0.
This is implemented by comparing the sparsity patterns of each ray pair in E(K i ) and removing any ray r for which there exists an r' such that NZ(r') ⊂ NZ(r).
On the other hand, as illustrated in Figs. 2 and 4, each ray affects multiple regions x i on the diffuser ({mathcal {B}}) in different positions and each region is also affected by multiple radiant intensities s j.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com