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Due to the distance dependence of the interference, in order to derive expressions for the above terms, we apply the concept of guard zones [10].
In Figure 5 we show the dependence of the interference peak maxima number on the inverse of the wavelength for the two samples of Figure 4, the color code being also the same.
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We can see from this expression that, for the non-squeezing case ((s_0=1)), the time dependence of phase of the interference term follows ([q-Q_p(t)]P_{mathrm{t},c}(t)/rho (t)).
However, the dependence of interference (link suppression) on the degree of correlation between the regulators, the expression levels of the regulators and their targets, is unknown.
In addition, the dependence of interference on array electrode size has been investigated.
Averaging over a band of frequencies generally removes most of the interference effects, except for application points close to the far boundary, the remaining dependence on the application point being equivalent to the effects of mode shape coherence.
Minimization of the interference.
Figure 5 Dependence of the average sum rate (a) and of the average network congestion (b) on the self-interference coefficient.
From these curves we see that the expected lnT dependence of the resistivity is clearly observed until ∼0.3 T when the magnetic field is strong enough to break the quantum interference.
Figure 3 shows the dependence of the average sum rate (Figure 3(a)) and of the average network congestion (Figure 3(b)) on the self-interference coefficient.
Figure 5 shows the dependence of the average sum rate (Figure 5(a)) and of the average network congestion (Figure 5(b)) on the self-interference coefficient for SNR values 5, 16, and 30 dB.
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