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The relationships among members of the different STs and CCs are demonstrated in the Appendix Figure.
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These connections are demonstrated in the Appendices.
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.
As demonstrated in the online supplementary appendix, this leads unequivocally to the bound on Q used throughout this paper.
In this case, as demonstrated in appendix the noise level is increased (or decreased) by dB.
Thousands demonstrated in the streets.
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).
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).
We demonstrate this in the Appendix for an arbitrary tree with nodes of degree d = 3 or less.
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]).
The use of Eq. (23) is demonstrated in "Appendix 1".
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