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The measured filter passband insertion losses are less than 2.7 dB.
As the Faraday filter passband is narrow enough, the return lidar signals in both the resonance fluorescence and Rayleigh scattering are affected.
The Bessel filter is optimized to provide constant group delay in the filter passband, while sacrificing sharpness in the frequency response.
We find that there can be significant XPM-induced intensity distortion, especially near the edges of the filter passband where the in-band dispersion is increasingly pronounced.
It is assumed that the filter impulse response is normalized so that the mean input and output signal powers remain constant, if the incoming signal is contained in the specific filter passband.
With only two or three stages, the useable filter passband is broadened by more than two orders of magnitude compared to single-stage (e.g. Fabry Perot) filters thereby improving the robustness of the device to frequency detuning.
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The measured filters' passband insertion losses are less than 2.74 dB at central frequencies.
All signal intensity time-courses were bandpass filtered (passband 0.012 0.1 Hz) and orthogonalized with respect to the global mean brain signal.
This leakage is filtered through passband filtering, resulting in phase errors at the edges of the frame.In order to remove the phase errors, we adopt overlapping processing of the FFT frame.
In the first case, the filter length, passband and stopband frequencies, and the ratio of the passband and stopband ripples size are specified.
It is worth noting that the error probability is approximately in the majority of channels belonging to the transition band, which is approximately between channels and. Figure 12 WNR versus DFT channel for colored host and lowpass filter with passband rad and stopband rad. Figure 13 Ber versus DFT channel for colored host and lowpass filter with passband rad and stopband rad.
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