backscatterers distributed over the cell. The amount
of energy backscattered by these individual
scatterers can be equal or can vary and the
positional distribution of them is regular or
irregular. In a non-homogeneous cell the dominant
scatterers will have the highest influence on the
phase, therefore variation in the position of
dominance will vary the phase significantly. These
points with a relatively high response (figure 1)
will also have a too large influence on the
computation of the coherence map (figure 2). This
influence can be reduced by means of a filter
combination as described in this paper.
Apart from temporal changes, decorrelation can
also be a consequence of an improper (too large)
distance (base) between the two sensors during the
data acquisition. In case of the extraction of
thematic information, the decorrelation related to
the base line should be minimized such that
Figure 2 Coherence map of The ERS-1/2 pair
differences that appear can be considered to come
mainly from temporal decorrelation.
1.1 Coherence
The complex coherence between two SAR images
is defined by (Touzi et al., 1996):
E\S, - 55)
E IS E IS,
and the estimator of the coherence is defined by
M
: . 5146
RS a; a, -¢€
^ izl
SC i y : T (a5; y
izl izl
For each map element, the coherence is computed
in a window surrounding that point. The value
between 0 and 1 is related to the equality of the bi-
directional signal of the two sub-images (from
master and slave). A constant phase shift between
the corresponding elements of the images does not
modify that value. In the computation of the
coherence, by the above given formula, is the
contribution of such a constant phase shift
eliminated.
However, the influence of a strong backscatterer
(e.g. a corner reflection) is dominant in its
surrounding in the computation of the coherency.
This dominance results in a high coherence over a
larger area than in reality the case. For example, an
element in a sub-image of the same size as the
kernel of the (filter) operator (40 * 7 elements)
represent a very strong scatterer (e.g. thousand
times the scatterers in its surrounding in both the
ERS-1 and the ERS-2. This strong scatterer will
overrule the other elements at a distance smaller
than the kernel size. That means that a large kernel
(e.g. 150*150meter in ground size) shows a very
high coherence over that area without being
realistic.
If the coherence map is used for thematic
information extraction, then important information
can be hidden by this way of coherence
computation. The images in figure 3 visualize this
Intemational Archives of Photogrammetry and Remote Sensing. Vol. XXXII, Part 7, Budapest, 1998
539