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Next: Examples for interpolators Up: Evaluation of interpolation kernels Previous: Introduction

Theory of interpolation errors

The following analysis starts from the classical Fourier domain description of interpolation errors in stationary signals. Often these errors are quantified in terms of an L tex2html_wrap_inline470 norm. We will instead employ coherence theory for SAR interferograms [1][2] to predict the effect of interpolation on interferogram phase quality. Figure 1 shows (for the 1-D case) how the Fourier transform I(f) of a kernel i(x) acts as a transfer function on the periodically repeated signal power spectral density tex2html_wrap_inline476 . The two classes of errors to be considered are: the distortion of the useful spectral band tex2html_wrap_inline478 , and the insufficient suppression of its replicas tex2html_wrap_inline480 , where tex2html_wrap_inline482 is the sampling frequency. Hence, the interpolated signal will not be strictly lowpass limited and the subsequent new sampling creates aliasing terms. If in the resampling process all inter-pixel positions are equally probable, the aliasing terms are superposed incoherently and can be treated as noise with a signal to noise ratio of:

  equation38

In the following we will quantify interpolation errors in terms of interferogram decorrelation and associated phase noise. We assume that the original data tex2html_wrap_inline464 has been sampled at least at the Nyquist rate and that the sampling distance after resampling is similar to the original one.

   figure48
Figure 1: Fourier transform I(f) of interpolator i(x) acting on the replicated signal spectrum

The system model of figure 2 is sufficient for our analysis: consider a perfect and noise free interferometric data pair of coherence tex2html_wrap_inline490 , before interpolation. Both tex2html_wrap_inline464 and tex2html_wrap_inline466 have passed the SAR imaging and processing system described by a transfer function H(f). Signal tex2html_wrap_inline464 additionally suffers from the interpolation transfer function I(f), and alias noise n. It can be derived from [1] and [2] that for circular Gaussian signals (i.e. for distributed targets) the coherence of such a system is given by

  equation58

These equations are readily extended to two dimensions. If both tex2html_wrap_inline504 and tex2html_wrap_inline506 are separable, we find:

equation66

The phase noise resulting from tex2html_wrap_inline508 is known to be (in the N-Look case):

equation68

where

eqnarray73

and tex2html_wrap_inline512 is the Hypergeometric function.

   figure83
Figure 2: System model for evaluating interpolation errors (w is a white circular Gaussian process)


next up previous
Next: Examples for interpolators Up: Evaluation of interpolation kernels Previous: Introduction

Ramon Hanssen
Wed Jan 28 18:12:38 PST 1998