Parallel Doppler (Ndop = 3)


Parallel Doppler methods may be visualized as a set of coherent stacking operations carried out at offset Doppler frequencies (Raney, 1998b). Three new steps are required: (1) sorting the data into Doppler bins, (2) delay compensation, and (3) parallel Doppler summation. Consider these in turn.

(1) Doppler bins. The sounder is operated coherently as in coherent stacking, and a sequence of undetected return waveforms is stored in memory. This is a two-dimensional data array: delay, and pulse number. When a complete group of returns has been collected, the data are transferred to a processor for operations while the next group accumulates. In the processor, an along-track fast Fourier transform (FFT) at each delay increment integrates over the sequence of pulses. The data are thus transformed into another two-dimensional data array: delay, and Doppler frequency. It is convenient to use a power of two for group size. For this example, there are 32 pulse returns in the input group, and the data are sorted into 32 output Doppler bins.

(2) Delay compensation. Within each group, Doppler frequency corresponds to a scatterer's position along-track relative to nadir, where nadir maps into the zero-Doppler bin. At all non-zero Doppler bins, there is an extra delay due to its off-nadir location. The loci of these extra delays are hyperbolae, evident in the incoherent average example. The extra delay at each Doppler is known from the sounder's geometry. Therefore, this extra delay can be removed, for which there are several means to do so (Raney, 1998a). After delay compensation, the waveform depths within all Doppler bins are in agreement.

(3) Parallel Doppler summation. The delay-compensated output waveform in each Doppler bin is square-law detected. Recall that each Doppler bin for each group corresponds to a particular along-track position. Thus, the trick in parallel Doppler summation is to correctly select the corresponding waveforms across groups. Each completed output waveform is the summation across Ndop Doppler bins, where 1 < Ndop <= 32 for this data set.
The example of this figure is for Ndop = 3, or summation over the zero-Doppler bin and its two adjacent neighbors. In this case, the SNR and the SSR are approximately 3 times larger than that observed in the coherent stacking example.


Keith_Raney@jhuapl.edu    Robert_Jensen@jhuapl.edu    Bruce_Gotwols@jhuapl.edu

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