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Repeating the same reasoning as that of Section 4.7, analogously to eq. (4.48),
search for the sets of vectors x solving the two-parameter equation in the n -
dimensional vector x :
x T A T Ax 2 b T Ax + b T b 2 γ( 1 ζ) 2 γζ x T x = 0
(5.43)
Similar to eq. (4.50), the center of the hyperconic x c is given by
x c , ζ ) = A T A 2 γζ I n 1 A T b
(5.44)
which, using the EIV decomposition (4.52) of A T A , becomes
V
I n 1 q
x c
,
ζ ) =
2
γζ
(5.45)
As in eq. (4.51), the following two-parameter equation in the n -dimensional
vector y , without first-order terms, is obtained:
y T A T A 2 γζ I n y b T A A T A 2 γζ I n 1 A T b + b T b 2 γ( 1 ζ) = 0
(5.46)
By using eq. (4.52), eq. (5.46) becomes
y T V (
V T y
b T AV
2 γζ I n 1 V T A T b + b T b 2 γ( 1 ζ) = 0
2
γζ
I n
)
(5.47)
By introducing
g , ζ ) = b T AV 2 γζ I n 1 V T A T b b T b + 2 γ( 1 ζ)
(5.48)
the equations corresponding to eqs. (4.56) and (4.58) are
z T 2 γζ I n z = g , ζ )
(5.49)
and
n
q i
ζ) b T b = q T
g
,
ζ ) =
λ i 2 γζ +
2
γ(
1
i =
1
I n ) 1 q
b T b
(
2
γζ
+
2
γ(
1
ζ)
(5.50)
respectively. Again, for any ζ , one and only one value γ min of γ exists in the
interval ( 0, λ n / 2 ζ ) such that g min , ζ) = 0. This point corresponds to the unique
minimum of the cost function E GeTLS EXIN ( x ) , with position given by
x GeTLS sol = x c min , ζ ) = A T A 2 γ min ζ I n 1 A T b
(5.51)
Figure 4.15 is also valid for the GeTLS problem if σ 2
is replaced by λ i / 2 ζ .
i
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