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where
is a scale factor. This binary quadratic optimization is known to be np -hard
[SM00], and its solution can be approximated by spectral relaxation
σ
Z T HZ
Z T Z ,
Z =
arg max
Z
Z
R .
(13)
Thus, Z is given by the eigenvector corresponding to the largest eigenvalue
λ 1 ,as
this maximizes Eq. 13. This approach can be considered as normalized cut cluster-
ing applied to the set of correspondences c i k j k N 1 N 2
. Namely, we assume that the
1
true correspondences c i k j k M
N 1 N 2 ) form a tightly connected cluster based
on the affinity measure in Eq. 12. In [CSS07] Cour and Shi proposed a doubly-
stochastic normalization of the affinity matrix H , and adding an affinity constraint
over the solution Z to enforce one-to-one matchings.
Given the relaxed solution Z , we apply the discretization procedure given in
[LH05] to derive an approximation Y to the binary vector Y . Note that since we are
interested in symmetry analysis, we expect to recover multiple solutions (eigenvec-
tors)
( M
1
Y i K
1 ,where K is the order of symmetry. In the following section we show
how to estimate K based on the eigenvalues of the affinity matrix H , and how to
recover the symmetry correspondences. We then compute the symmetry centers for
rotational symmetry, and axes of reflection for reflectional symmetry.
4
Spectral Symmetry Analysis
In this section we apply the spectral matching to symmetry analysis and derive the
spectral symmetry analysis scheme. We start in Section 4.1, by presenting a gen-
eral computational approach for the detection and analysis of symmetries of sets of
points in n-dimensional spaces. We then elaborate on the analysis of symmetry in
two-dimensional images in Section 4.2.
n
4.1
Spectral Symmetry Analysis of Sets in
R
n , with a symmetry of order K , it follows by Section 2, that
there exists a set of symmetry transformations,
Given a set of points S
R
,thatmap S to itself.
The main issue is how to detect these multiple transformations simultaneously. In
terms of numerical implementation, this implies that one has to look for a set local
solutions of the corresponding optimization problem. Most matching and alignment
schemes, such as RANSAC and ICP, lock on to a single optimal alignment, and it is
unclear how to modify them to search for multiple solutions.
Spectral relaxation provides an elegant solution to this issue. The multiple self-
alignments will be manifested by the multiple maxima of the binary formulation
in Eq. 11 and its corresponding relaxation in Eq. 13. The maxima of the Reigh-
ley quotient in Eq. 13 are the leading eigenvalues of the affinity matrix H ,and
the corresponding arguments are the corresponding eigenvectors. This beautiful
{
T C K }
and
{
T D K }
 
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