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If we consider an extraordinary wave (TM polarized) in a uniaxial medium, this isofrequency relation changes to k x 2 + k y 2 ε zz + k z 2 ε xx = ω 2 c 2 (1) Figure 1 Nanoscale Design.
where the elements of the matrix Ek,kare random variables, statistically independent of each other, each with variance σ e 2. Inserting Equation (14) in Equation (4), the input output relation changes to y k = H ̂ k, k + E k, k W k s k + n k + ∑ m ≠ k H k, m W m s m. (15).
Our starting relation changes to begin{aligned} gamma, overline{Phi }_1 iota (v) Phi _2 = (-1)^{|Phi _1|} iota (v) left( gamma, overline{Phi }_1 Phi _2 right) + (-1)^{|Phi _1|} varepsilon (overline{cv} gamma, overline{Phi }_1 Phi _2, end{aligned}since the operator (iota (v)) is an anti-derivation.
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Finally, the biggest impact on efficiency in our investigation was in relation to changes to sensor pairing (i.e., varying patterns between conditions).
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Furthermore, in four patients, the bilateral transversal relation changed from end-to-end to a bilateral crossbite.
In four patients from the oral appliance group, the bilateral transversal relation changed from normal to end-to-end and in one patient only the right side transversal relation changed from normal to end-to-end.
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