The sensitivity and phase curves of the loop antenna for ATH in Figs. 12 and 13 were measured for the maximum gain volume of the pre-amplifier and 20 dB gain (defined as no attenuation) for the volume of the main amplifier.
First, a characteristic that is relevant to an AQP technique (i.e., a characteristic that is monitored during the first phase of the adaptivity loop) is realized as a random variable or even as a collection of random variables.
Thus, the phase of the open loop transfer function is constant with respect to the inertia constant, while increasing the inertia constant will decrease the amplitude frequency gain and this stabilizes the system.
A region comprising the tandem PAS domains of PER has been found to interact with the PAS-containing regions of individual CLOCK and BMAL1 proteins by co-IP and is generally presumed to represent the basis for recruitment of PER CRY complexes to CLOCK BMAL1 early in the repressive phase of the feedback loop.
A Bode plot is the representation of the magnitude and phase of the open-loop transfer function of a system, where the frequency vector co-contains only positive frequencies.
With increasing temperature, the anisotropy field of CoFe2O4 decreases markedly, so the average reversal fields of hard and soft phases may be similar, resulting in the single-phase behavior of the loops (not shown here).
In addition, an automatic phase control loop has been included to adjust the phase of the main feedback loop to ensure an operating point as close as possible to the resonance frequency, which results in improved frequency stability.
The above rationale is incorporated in a novel monitoring phase which enhances the state-of-the-art one [9], while keeping the rest phases of the adaptivity loop unaltered.
CN precedes looping and the direction of the CN slow phase is predictive of the looping direction, but is absent during looping.
