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n
3
n
2
u
2
u
2
u
2
+
…
+
+
+
n
2
n
2
n
2
n
3
n
3
n
3
=
A
n
1
u
3
u
3
u
3
n
1
n
n
1
1
u
1
u
1
u
1
Fig. 9.5 Illustration of the CP-decomposition for a 3-mode tensor A. The
dashed lines
indicate the
boundaries of a rank-k factorization
Here, the symbol “
” represents the outer vector product, i.e., each element of a
∘
¼ v
i
i∈
n
k
, which is called a
CP rank-1-
tensor
, is the product of its corresponding vector elements
tensor
A ¼ v
1
v
d
with vectors
v
k
∘
...
∘
a
i
1
,
...
,
i
d
¼ v
i
1
v
i
2
...
v
i
d
:
Thus, we may write (
9.7
) component-wise:
a
i
1
,
...i
d
¼
X
t
u
i
1
,
j
u
i
d
,
j
:
j¼
1
Therefore, (
9.7
) tells us that each CP-tensor may be represented by a sum of
rank-1 tensors (Fig.
9.5
).
For
d ¼
2, the HOSVD, i.e., the “classical” SVD, coincides with a
it is not the identity matrix, we may multiply the diagonal values into the matrices
of singular vectors, for example, into
V
k
.
Example 9.7
The rank-2 approximation from Example 8.4 may be written as a sum
of two rank-1 tensors:
0
@
1
A
,
10
:
3
0
:
23
2
:
76 9
:
65
5
:
17
A
k
¼XY ¼
0
:
2
0
:
7
0
:
69
6
:
61
:
65
0
:
14
:
1
0
:
0
7
0
@
1
A
0
@
1
A
1
0
3
0
0
:
¼
:
2
ð Þ
|
{z
}
u
ðÞ
0
:
23 2
:
76 9
:
65 5
:
17
þ
:
7
ð Þ
|
{z
}
u
ðÞ
0
:
69
6
:
61
:
65
0
:
14
0
:
1
0
:
7
T
T
|
{z
}
u
1
|
{z
}
u
1
¼u
1
∘
u
1
þu
2
∘
u
2
:
■