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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
,
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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