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Recast z n as
z n Gq n
(5.83)
where
b T b
q n
G =
(5.84)
It follows that
G > H
(5.85)
Indeed, using property (5.68),
b T b + λ n
b T b + λ n
q n + λ
b T b
q n
H = 2
q n <
<
= G
(5.86)
λ
n b T b
+
2
λ
n
+
n
Hence, z n > | z n | .
It is easy to extend the inequalities to the other z components. Indeed, i =
1, ... , n ,
$
z i
q i
λ i
q i
λ i λ n + H 1
q i
λ i 2 γ min ζ I n
( z i )
z sol i min , ζ ) =
(5.87)
%
λ i λ n + G 1 z i
q i
Thus:
z i > z i because λ i λ n + G 1
i [ G 1
n for the property (5.68)].
z i > |
because G 1
H 1 .
z i |
<
| z i | > z i because λ i λ n + H 1
i . Indeed, | z n | > z n H 1
n .
These properties, a fortiori, justify eq. (5.80).
5.3.6 Existence of the OLS Solution and the Anisotropy
of the OLS Energy
A direct consequence of property (5.68) is the existence of the OLS solution.
Indeed, from eq. (5.50),
n
q i
b T b
g
min ,0
) =
λ i +
2
γ
=
0
(5.88)
min
i
=
1
iff b T b
and
the
zero
(energy
height
at
the
minimum)
is
nonnegative
i = 1 q i i (i.e., the above-mentioned property).
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