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We have demonstrated (Appendix 3 in Supplementary Material) that the CLIP test is consistent (that is, power of the test is 1 when grows to infinity).
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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).
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.
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]).
Also, empirical computations indicate that there is a 41.3 % probability that an extant entrepreneur who is generating revenue sees high chance of success (Table 7, following computations demonstrated in Appendix 2 (b)).
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.
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