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The received pulse is time-limited and band-limited.
At D, a received pulse waveform matched filter is employed.
The received pulse causes the oscillator to fire early.
The received pulse with the normalized amplitude is shown in Fig. 10.
(2) Multi-sourced interferences may contaminate some portions of the received pulse seriously.
Fig. 1 The sketch map of the received pulse reflected only with human respiratory.
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As noted for case 4, the measurement matrix is equal for all received pulses and receivers, i.e., ( boldsymbol{T}={boldsymbol{I}}_{M_r}otimes boldsymbol{varphi} ).
For such tags identified when the received pulse-burst exceeds a threshold, we specify the generic identification (ID) error probability and optimize the threshold employing the Marcum Q-function of first order.
Based on angle-Doppler estimates, the range is then estimated using frequency-varying received pulses.
In this case, the measurement matrix is equal for all received pulses.
In refractory, when with, no phase increment is possible, so that received pulses are not acknowledged.
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