where Ω
in
and Ω
out
are respectively the foreground
(targeted object) and the background areas, Γ the
evolving boundary between Ω
in
and Ω
out
and ξ
in
, ξ
out
and β three positive weighting parameters. Consid-
ering now the standard level-set embedding function
U of J
α
, the Lagrangian minimization scheme of J
α
leads to the following associated PDE for active con-
tour evolution:
∂U
∂t
= δU
β∇·
∇U
|∇U|
−
ξ
in
|Ω
in
|
(A
in
−C
in
)
+
ξ
out
|Ω
out
|
(A
out
−C
out
)
, (4)
with
A
i
= ∂
1
ϕ
α
( ˆq(λ, Ω
i
), p
i
(λ)) ∗ g
σ
(I(x)), (5)
C
i
=
Z
ℜ
∂
1
ϕ
α
( ˆq(λ, Ω
i
), p
i
(λ)) ˆq(λ, Ω
i
)dλ,
where i = {in, out} and ∂
1
ϕ
α
denotes the first deriva-
tive order of ϕ
α
function with respect to ˆq, g
σ
is the
Gaussian kernel (with standard-deviation σ) used in
the Parzen window estimation of ˆq, I is the intensity
function of the segmented image at a pixel x. The
implementation of Eq. (4) is achieved with a semi-
implicit version of the Additive Operator Splitting
scheme.
3 EXPERIMENTAL RESULTS
In order to achieve the automatic segmentation of
both nuclei and cell boundaries, inner and outer refer-
ence PDFs, corresponding to the targeted structures,
are computed applying a standard three class (for
cell boundaries, cytoplasm and nucleus) Expectation-
Maximization (EM) algorithm on the equator slice
of the PNT2 acquisition. This rough classifica-
tion is good enough to define the reference PDFs
using Parzen window technique: the strategy is
then one class (“nucleus”, resp. “cell boundaries”)
against the two others (“cell boundaries+cytoplasm”,
resp.“nucleus+cytoplasm”). The segmentation pro-
cess is initialized on the equator slice (Fig. 1 mid col-
umn) through the monolayer. For both nuclei and cell
boundaries segmentations, the zero level-set initial-
ization of the function U
0
is given as a set of small
circles uniformly distributed across the whole slice.
Finally, the segmentation process is spread all along
the different slice level of the monolayer.
Fig. 1 summarizes results obtained for different
slices from the acquired 3D image stack and for dif-
ferent values of the parameter α. All tests are done
with the same optimal parameters ξ
i
(here ξ
in
= ξ
out
)
and β for both nuclei and cell boundaries (empirically
tuned on the equator slice image) in order to focus on
analysis the influence of the α parameter only.
Considering nuclei segmentation, as shown in
Fig. 1 in green, thanks to the level-set formulation
and to the integration of alpha-divergence measures,
all nuclei are detected during a single run of the algo-
rithm, even those with incomplete shape (at the bor-
der of image). This is a major advantage when com-
paring with the Chan-Vese approach which needs to
be carefully adapted (in its regularized form) to per-
form the same task as shown in some of our previ-
ous work (Meziou et al., 2011) on that topic. It is
also important to notice that the more accurate results
are obtained with non-standard values of α as shown
in Figs. 1. (b). where α = 0.75. The real difficulty
is to obtain a robust segmentation result of each nu-
cleus to avoid small structures segmentation within
cytoplasm reflecting the complexity of the cytoplasm-
nucleus boundary. For the higher values, false detec-
tions could appear and non significant small structures
are segmented as shown in Figs. 1. (e).
For each slice segmentation, an expert can man-
ually suppress false detected nuclei that can occur
when a hole representing an empty space between
cells is present in the cell culture for instance: Sta-
tistically speaking, the PDF of a hole is very close to
the PDF of a nucleus and can be difficult to differen-
tiate automatically.
In the case of cell boundaries, shown in red in
Fig. 1, segmentation is more demanding since even
for experts it is not always easy to visually identified
them: the non-homogeneity of the actin fluorescent
marker can strongly influence the pixel levels corre-
sponding to cell boundaries which could explain dif-
ficulties to get continuous contours. Results obtained
are similar to those obtained with Chan and Vese seg-
mentation which performed well for this particular
task and can be considered as a reference for that kind
of single channel acquisition. However, major advan-
tage of the proposed approach for cell boundaries seg-
mentation is the use of the same evolution criterion
(alpha-divergence measure) for both cell boundaries
and nucleus segmentations. Influence of the α param-
eter, as for nuclei segmentation, is interesting since
it can be noticed again that the most interesting re-
sults are obtained for a value of α that does not cor-
respond to standard histogram distance measures. In
terms of cell boundaries segmentation, the proposed
results have to be considered as prospective ones but
very encouraging. From an expert point of view, the
best results are obtained for a high value of α (for ex-
ample α = 1.5 shown in Figs. 1.(d)).
3D CONFOCAL MICROSCOPY DATA ANALYSIS USING LEVEL-SET SEGMENTATION WITH ALPHA
DIVERGENCE SIMILARITY MEASURE
407