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relating again to the simultaneous diagonalization of two matrices, e.g. the pairs of Cauchy-Green
deformation tensors
{
C
l
,
G
l
}
or
{
C
r
,
G
r
}
and the pairs of Euler-Lagrange deformation tensors
{
. respectively. Of course, we could also aim at a simultaneous diagonalization
of three matrices, e.g. the triplets
E
l
,
G
l
}
or
{
E
r
,
G
r
}
{
E
l
,
C
l
,
G
l
}
versus
{
E
r
,
C
r
,
G
r
}
,
(2.70)
in particular
U
l
G
l
X
l
=S
l
⇔
G
l
=U
l
S
l
X
−
1
versus G
r
=U
r
S
r
X
−
1
⇔
U
r
G
r
X
r
=S
r
,
(2.71)
i
r
X
l
C
l
Y
l
=S
l
⇔
C
l
=(X
−
l
)
T
S
l
Y
−
l
versus C
r
=(X
−
r
)
T
S
r
Y
−
1
X
r
C
r
Y
r
=S
r
,
⇔
(2.72)
r
Y
l
E
l
V
l
=S
l
⇔
E
l
=(Y
−
l
)
T
S
l
V
l
versus E
r
=(Y
−
r
)
T
S
r
V
r
⇔
Y
r
E
r
V
r
=S
r
,
(2.73)
where S
1
,
S
2
,andS
3
are certain quasi-diagonal matrices, where V and U are unitary matrices.
and non-singular matrices are X
l
,
Y
l
and X
r
,
Y
r
, respectively. But we are not able to diagonalize
G
l
and G
r
, respectively, to unity. The diagonalization of G
l
and G
r
, respectively, to unit matrices
is by all means recommendable since accordingly all other tensors, e.g. C
l
and C
r
, respectively,
or E
l
and E
r
, alternatively, refer to unit vectors which span the local tangent space of
M
l
or
M
r
, respectively. Before we proceed to the next chapter, let us here additionally note that a
tree of generalization of the ordinary singular value decompositions has been developed by
Chu
(
1991a
,
b
),
De Moor and Zha
(
1991
),
Zha
(
1991
), and others to which we refer.
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