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Thus, the general form of the
barrier locus
is given by
2
q
j
v
j
x
bar
≈
±
(5.102)
λ
−
2
γζ
j
The same considerations of the two-dimensional case can be applied here. In
particular, the following theorem results.
Theorem 106 (Barrier Asymptotic Behavior)
The GeTLS convergence bar-
rier asymptotically follows the z directions
(
i.e., the directions of the
v
j
eigenvec-
tors for j
=
n
)
.
5.3.8 Critical Loci: Center Trajectories
Equation (5.45) represents the locus of the centers of the equilevel hypersurfaces
in the
x
reference system; in the
z
reference system, rotated by the matrix
V
around the origin, this equation becomes
ζ )
=
−
I
n
−
1
q
z
c
(γ
,
2
γζ
(5.103)
that is, for each component (
i
=
1,
...
,
n
),
q
i
λ
i
−
2
γζ
z
ci
=
(5.104)
In each plane
z
j
z
i
this locus is an equilateral hyperbola translated from the origin:
q
i
z
j
λ
i
−
λ
j
z
j
+
q
j
z
i
=
(5.105)
All these loci pass through the
z
origin, which coincides with the
x
origin. Its
asymptotes are given by
q
j
λ
q
i
λ
z
j
=−
and
z
i
=
(5.106)
where
λ
=
λ
i
−
λ
j
.
Definition 107 (Asymptotes)
The asymptote of the hyperbolas parallel to z
i
(
the coordinate along the direction of the eigenvector
v
i
associated to
=
σ
2
i
λ
i
)
is defined as the z
i
asymptote
.
Assuming distinct singular values for
A
, these loci tend to degenerate into two
corresponding orthogonal straight lines for
q
j
→
0or
q
i
→
0.
The global locus (5.104) is parameterized by the product
γζ
. The parameter
t
=
2
γζ
will be used [see eq. (5.74)]. If a priori assumptions are not made, the
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