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*
() =d
vv
.
i
j
ij
The map from V to V * that sends v i to v i * is a vector space
C.5.2. Theorem.
isomorphism.
Proof.
Straightforward.
The isomorphism in Theorem C.5.2 between V and V * clearly depends on the
basis.
The basis v * , v * ,..., v * is called the dual basis of v 1 , v 2 ,..., v n .
Definition.
Notice that if
n
 a ii
i
wv
=
,
=
1
then v i *( w ) = a i , so that the ith dual basis element just picks out the ith component
coefficient of the expansion of a vector w in terms of the v i 's.
C.5.3. Theorem. Let V and W be vector spaces over a field k and let T : V Æ W be
a linear transformation. The map
T* :
WV
*
Æ
*
defined by
( () =
(
()
)
T
*
a
v
a
T
v
,
for
v
Œ
V
,
is a linear transformation.
Proof.
Easy.
Definition.
The map T* in Theorem C.5.3 is called the dual map of the linear trans-
formation T.
Next, given v ΠV , define v ** ΠV ** = ( V *)* by
() =
()
v
**
aa
v
,
for
a
Œ
V
*.
C.5.4. Theorem. The map from V to V ** that sends v to v ** is a vector space iso-
morphism called the natural isomorphism between V and V **.
Proof.
Easy.
Note that, although the isomorphism between V and V * depended on the choice
of a basis for V , the isomorphism between V and V ** does not. This allows us to iden-
tify V ** with V in a natural way and one often makes this identification.
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