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The optical link exhibits good linearity (to within 12%) over a large dynamic range of 61 dB with an acceptable amount of pulse-shape and harmonic distortion across the entire bandwidth of ∼250MHz, which is itself limited by the response of the receiver.
Then, we calculated the frequency response of the receiver by calculating Eq. (8). Figure 13 shows the pre-launch results of the SWCAL function.
The frequency response of the receiver will then be characterized by the amplitude and the phase of the kinematic solutions obtained from the GPS observations.
On the other hand, in order to obtain the response of the receiver, we input the receiver calibration signal,, by using one-to-eight power divider with the response of.
The kinematic solutions were calculated from the GPS observations for each test signal input individually, and the frequency response of the receiver was obtained directly from the amplitude and phase difference between the kinematic solutions and the true antenna motion.
As mentioned earlier, the actual PLL inside the receiver is not strictly a linear system, and the peak jerk stress obtained from Eq. (4) may not guarantee the dynamic response of the receiver.
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The main goal of constructive criticism is to deliver a nuanced response to the receiver.
As is much smaller than, the variation of the phase error over the impulse response duration of the receiver filter can be safely neglected.
Given that the Sender does not differentiate states of the world 2 and 3, the Receiver cannot improve his payoffs by responding differently to signal 2. Given the particular response behaviour of the Receiver, the Sender cannot improve her payoffs by attempting to differentiate states of the world 2 and 3.
In addition to the modulating signal and the instantaneous total power response of the quadrature receiver, the first two time derivatives of the modulating signal are also shown.
Since the effect of the antenna impedance is ignored when (R_{{mathrm{CAL}}}) is selected to (1,{mathrm{k}}Omega), we can measure the end-to-end frequency response of the WFC receiver including the preamplifier [see Kasahara et al. (2018) in this issue].
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