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By the approach in the preceding sections, for the Neumann problem, the results are as follows.
Here we consider another variation of the results derived in the preceding sections.
Several points can be outlined in relation to the techniques discussed in the preceding sections.
Finally, Section 5 is devoted to summarizing the work presented in the preceding sections.
This assumption was used in the analysis for CM-DM processing in the preceding sections.
Otherwise we leave all the other definitions stated in the preceding sections unchanged.
In this section, we briefly consider another variation of the results derived in the preceding sections.
They were discussed accordingly in the preceding sections of this study.
The beam was then re-retested as described in the preceding sections.
In this section, we compare the performance of the methods presented in the preceding sections.
This basic principle will be used to verify the SIR bounds derived in the preceding sections.
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