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The phase response has a maximum phase shift of 2.88 rad at 0.1 Hz, as shown in Figure 3b.
Phase is controlled by varying DC voltage on a varactor, resulting in 60° maximum phase shift with 0.1 dB amplitude variation at 24 GHz.
The design is based on a well-known RC bridge topology, which was optimized for maximum phase shift and minimal amplitude response variation versus phase and frequency.
This is in contrast to phase shifting transport approaches, where the maximum transport distance is given by the maximum phase shift [60].
The same is reflected in the change of phase angle, where the maximum phase shift (Φ = 61°) obtained in G-CNTs at frequency of ~1.0 Hz is moved to a high region (>100 Hz).
As a result, the maximum phase shift (observed at zero elevation), Ψ max = kd cos ϕ, lies between 6π and 10π, while instrumentally the phase can only be measured between −π and +π. Figure 2 shows the relationship between elevation and phase shift for central beams (φ = 0) at the typical Hokkaido East frequency of 11 MHz.
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We have shown that such networks respond in fact opposite, and show a maximum phase shifting capacity when the rhythm amplitude is large, and a smaller response when the amplitude is low.
Moreover, these studies used very bright light to obtain maximum phase-shifting.
Therefore, without phase unwrapping, the maximum detectable phase shift is π, and the maximum detectable axial velocity is given by The theoretical limit for the minimum detectable velocity, on the other hand, is determined by the phase stability of a PR-DOCT system.
Bode impedimetric analysis indicates that Pt|G2PPI-co-PPy isemiconductorctor with a maximum phase angle shift of 45.3° at 100 MHz.
The opposite is true of circular coils, with a maximum negative phase shift of minus 5.5°.
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