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Due to the high impurity radiation power (80% of the exhausted power), the full detachment at the inner target and the partial detachment at the outer target are obtained for a relatively low electron density of 1.8 × 1019 m−3 at the outer mid-plane separatrix.
Once the Doppler parameters of each target are obtained, substituting them into Eq. (23), we can get the v x v y = ( v a - v x ) x o R o - λ f d c 2 ≈ v a x o R o - λ f d c 2. (41).
To get automatic point registration, we use a random method to produce the controlling points for TPS, in which a mount of controlling points are generated randomly in the reference and its correspondent points on the target are obtained by ICP closest points searching method.
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The composite target is obtained by addition of Pd tiles on top of a Fe target.
Profiles of output photon beam on the target were obtained.
The beam profile at the target is obtained using a simulation.
Several different application examples are given, and the target is obtained with high uniformity and energy efficiency.
Track of moving target is obtained.
Combined with the SPWVD time-frequency technique, the instantaneous Doppler frequency of the target is obtained.
The MAPLE target was obtained by dispersing nanoparticles in aqueous or saline solution.
In the first type, the returned signal of each target is obtained by parameter separation [10 13].
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com