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The use of Eq. (23) is demonstrated in "Appendix 1".
In this case, as demonstrated in appendix the noise level is increased (or decreased) by dB.
At high SNR, it is also demonstrated in Appendix Appendix 2: BER of a MISO system using EGT that lim ρ → + ∞ BER ¯ EGT = 1 16 σ 4 1 ρ 2 = 1 4 1 ρ 2 (25).
It is demonstrated in Appendix 2 that the MC of A is equal to mu left(mathbf{A}right)=mu left({boldsymbol{Theta}}^Tright) mu left(boldsymbol{B}right) (41).
In a broad sense, the obtained curves confirm what is mathematically demonstrated in Appendix, that an MMSE will provide a very high equalization weight when is exposed to a null, and that will do the opposite thing for a peak.
We parametrize the source field jext with spherical harmonics Y n m (where n and m denote degree and order of the spherical harmonic, respectively), as demonstrated in Appendix G of Kuvshinov and Semenov ([2012]).
Similar(53)
However, as demonstrated in Appendices B-1 and B-2, any degree of DC impairments associated with PIP or MCP joints of the index, middle, ring, or little fingers can be calculated using the algo- rithms presented here.
The cantilever with the mirror and the target units as a vibrating system can be treated by means of the Euler-Bernoulli beam theory, e.g. [25], which is demonstrated in this Appendix.
The relationships among members of the different STs and CCs are demonstrated in the Appendix Figure.
These connections are demonstrated in the Appendices.
As demonstrated in the online supplementary appendix, this leads unequivocally to the bound on Q used throughout this paper.
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