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However, the optimum scanning order differs for each video sequence.
Thus, in the decoder, the optimum scanning order cannot be obtained before the decoding process completes.
The optimum scanning order can be obtained by searching the transform coefficient i that minimizes the above formula for each bitplane from 1 to N.
The variable which grants maximum difference is selected for imaging while measurement conditions associated with this maximum indicate optimum scanning conditions.
As can be seen, the proposed bitplanewise zigzag scanning method provides close performance to that for the optimum scanning method and much better performance than the coefficient scanning method.
This creates difficulties in establishing an optimum scanning time as the half-life of the radioisotope must also be considered (110 min for F).
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Therefore, the optimum scan rate has been found to be 70 mV?s?1.
The results showed the high surface area as well as high connectivity between particles resulted at optimum scan rate.
The optimum scan is obtained using a Lagrange multiplier given in Eq. (7) to maximize the rate distortion performance for the entire test sequences and it represents the upper bound of rate distortion.
Optimum laser power, scanning speed and laser beam diameter was 150 W, 1500 mm·min− 1 and 2 mm, respectively.
The absorption spectra of the coloured complexes under optimum conditions were scanned in double beam mode against a reagent blank over the range 400 900 nm, and recorded according to general procedures.
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