International Archives of the Photogrammetry, Remote Sensing and Spatial Information Science
larly, i.e. they are better correlated with each other. The sur
face appears smoother and more realistic. The. modelled
scene radiance (Fig. 2d) can hardly be distinguished from the
original ortho-image (Fig. 2a). There are, of course, differ-
ences caused by the limitations of the present program ver-
sion. The somewhat brighter appearance of Fig. 2a as conr
pared to Fig. 2d is probably due to a slightly varying BRDF,
i.e. deviation of the actual reflectance law from Lambert. Fig.
2a also suggests two distinct regions with different albedo
factors. By applying only one albedo factor to the image data
this brightness difference has been evened out thus leading to
a duller and less bright result image. Further differences are
caused by the few small shadow areas, since shadows were
incorrectly treated as non-shadows.
A crucial point is the optimal value for the penalty factor. We
processed the data with a series of different values. The one
which intuitively and subjectively gave the most pleasing res
ult was considered optimal (0.005). We are, however, still
unable to comprehend its relationship with the underlying
stochastic model as given by Equ.(3). Yet, some statistics of
the differences between SFS-refined DEM and initial DEM
may give an indication of the significance of the result. Real
ize that pixel size is 232 m.
Maximum difference: 279 m
Mean difference: 0.46 m
Minimum difference: -265 m
Standard deviation: 32m
Fig. 3 exhibits the main processing stages of a 150 by 150
pixel subsection of an HRSC scene taken on 24 February
2004 at 266 km altitude in orbit 143. Approximate location is
137? W longitude and 40? N latitude in the Acheron Fossae
on the northern slope of Olympus Mons. The topographic
surface is therefore generally inclined towards North. .Illu-
mination is somewhat from the south with 48° sun elevation.
The ortho-image prepared by DLR is illustrated in Fig. 3a. It
has been radiometrically enhanced for better detail recogni-
tion. With 100 m pixel size the scene covers an area of 15km
by 15km. Printing scale is 1:400°000, hence more than 6-
times larger than that of the MOC image. The corresponding
DEM is shown as grey scale image in Fig. 3c. It was determe
ined by the DLR data processing group by image matching
(SFM) from the HRSC stereo channels at the original 30 m
resolution level. The modelled scene radiance (Fig. 3b),
however, shows enormous deficiencies in the DEM caused
mainly by insufficient surface texture needed for SFM. Real
ize that Fig. 3b is supposed to appear as Fig. 3a! The contour
lines of the SFM-determined DEM (Fig. 3d) may give an
idea of the difficulties SFM has had for matching the image
data.
Figs. 3e, 3f, and 3g show the same scene after SFS-refine-
ment after 10 CGM-iterations. Despite some unwanted (and
not yet comprehended) boundary effects visible mainly in the
contour map (Fig. 3g), the resulting scene radiance (Fig. 3e)
is much more alike the original ortho-image (Fig. 3a). AF
though there are — probably illumination induced — artefacts
visible in the DEM-image (Fig. 3f) and other errors due to in-
complete modelling, a dramatic improvement of the pure
photogrammetric, i.e. SFM-derived, DEM is obvious. As to
be expected (intuitively) the larger scale imposes more prob
lems for SFS concerning details. The shadow region along
the southern inside slope of the big impact crater exhibits er-
rors as well. Further improvenients may be expected in due
course with methodical expansions and refinements of DRS.
Fig. 3b,c,d:
Scene radiance, DEM im-
age and contour map prior
to SFS
Fig. 3e
Fig. 3e.f.g:
Scene radiance, DEM ima-
ge and contour map after
SFS-refinement
Fig. 3g
Figure 3. HRSC narrow-angle scene 15km by 15km
at printing scale 1:400'000
1302
s, Vol XXXV, Part B4. Istanbul 2004
Internation
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ACKNOWI
This work w
tion and Re:
the German .
The authors
members M:
Institute for ]
and unselfisl
for our rese.
Bernd Jeschk
portant conti
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Academy of
matters of op