Based on above analysis, a novel multi-scale Level Set method
is proposed for automatic extraction of water bodies. Compared
with single-resolution approaches, employing multi-scale model
for SAR image segmentation offers several advantages. Firstly,
multi-scale segmentation is a method considering both global
information and local information of the image, thus,
segmentation accuracy is increased. The overall structural
information of the image can be maintained at coarse scales and
detailed information can be kept at fine scales. Therefore,
coarser scale segmentation results can be used as a prior guide
for the finer scale segmentation, so that not only are the
statistical properties of the signal-resolution image considered,
but also statistical variations of multiple resolutions are
exploited. Secondly, computational complexity is reduced since
much of the work can be accomplished at coarse resolutions,
where there are significantly fewer pixels to process. Moreover,
OTSU algorithm (1979) is introduced to initialize the level let
functional; this simple technique brings significant
improvements in speed and accuracy. Finally, post-processing is
applied to segmentation result for removing some confused
objects.
2. PROPOSED METHOD
In this section, the basic principle of the proposed method is
outlined in Figure. 1. We acquire multi-scale images at several
scales by decomposing the SAR image using the block
averaging algorithm.
The principal steps of our algorithm are as follows:
1) Decompose the image into L scales by the block
averaging algorithm. Let K=L.
2) Use the OTSU algorithm to initialize the level set
function of scale L. Go to Step 3).
3) Obtain the scale-K segmentation result using the level
set method with the Gamma model.
4) K-K-l.
5) IfK--0, return to Step 2).
Blam t
p
Scale I.
Seat 6
Sfc vest
Figure.1 Basic framework of proposed method
2.1 Level set method based on gamma model
Chan and Vese proposed a model that implements the
Mumford-Shah functional via the level set function for the
purpose of bimodal segmentation. The segmentation is
performed by an active contour model without boundaries. Let
© be a bounded open subset of R?, with dQ being its
boundary. Let up (x, y) : © — R be a given image, and C be
a curve in the image domain (2 . Segmentation is achieved by
the evolution of curve C , which is the basic idea of the active
contour model. In the level set method, C C is represented
by the zero level set of a Lipschitz function $: (2 — R ; we
International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, Volume XXXIX-B7, 2012
XXII ISPRS Congress, 25 August — 01 September 2012, Melbourne, Australia
replace the unknown variable C by unknown variable @ ,
following Zhao et al. (1996).
Using the Heaviside function H , and the one-dimensional
Dirac function dy : defined, respectively, by
pei fI on EER €*
zz z)=—H(z t
pug vt e s
segmentation is performed by evolving $ such that it
minimizes the energy functional below:
F(ci.cs.9) 7 u |, 9G. DIV BO dd
+ jf, H (g(x, y)dxdy
&A [ eG) - a HGGs yay
+ À [ luo Gc y) - € P (1 — H(d(x, y)))dxdy
(1)
where ug is the given image, constants C, , C? are the
averages of ug(x, y) inside C and outside C , respectively,
and s. v. A x À, are non-negative weighted parameters.
Function @(x,y) represents class ©, for ÿ>0 , and
OQ» ford «0.
For SAR images, the probability density function (PDF) of the
pixel intensity is often given by a Gamma distribution. In this
work, considering the speckle noise, we model the image in
each region R; by a Gamma distribution of mean intensity 1;
and number of looks L :
Lug (x)
L
L (^ G2 14 or Q)
uj(L) uj
Puy (x) =
For scale images decomposed by bilinear interpolation, the PDF
of the pixel intensity is also given by a Gamma distribution.
This follows from Theorem 1.
Theorem l: For two given images ug(x) and u(X) , u(X) is
the decomposed image generated by bilinear interpolation. If
u(x) is modeled by a Gamma distribution, so is u(x) . Proof
of Theorem 1 is given in Section 2.2.
Therefore, the level set functional for SAR images can be
improved according to Equation (6) as follows:
F(o.P1.P2)= | VH(@dsdy +v| H(p)dsdy
=n [| H(p)log Pedy G)
- A5 [ (1- H(p)) log p,dxdy
The evolution of $ is governed by the following motion partial
differential equation:
ô V
2s, 9) TE v log p,(y|0,) + 4; logp; (3102) 4)
where J, (¢) is a regularized version of the Dirac function.