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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
(γ
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
<λ
i
[
G
−
1
<λ
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
<λ
i
. Indeed,
|
z
n
|
>
z
n
⇒
H
−
1
•
<λ
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
(γ
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
/λ
i
(i.e., the above-mentioned property).
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