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is denoted by L k ( V ). By convention, V 0 = 0 and L 0 ( V ) = R . There is an exterior or wedge
product
r
() ¥
s
() Æ
r
+
s
()
Ÿ
: L
VV
L
L
V
that is distributive and associative. (The classical notation such as dxdy is really an
abbreviation of dxŸdy.) Define
n
Â
() =
k
()
L
V
L
V
.
(4.25a)
k
=
0
Vector addition and the product Ÿ make L( V ) into an algebra called the algebra of
exterior forms on V ,
The defining properties of the algebra of exterior forms on V:
(1) If wŒL r ( V ) and hŒL s ( V ), then
1 rs
Ÿ= () Ÿ
wh
hw
.
(4.25b)
In fact, for any permutation s of {1,2, ...,k} and a i ŒL 1 ( V ), we have that
= (
)
aa
Ÿ
Ÿ
...
Ÿ
a
sign
s aa
ŸŸŸ
...
a
.
(4.25c)
( )
( )
(
)
s
1
s
2
s
k
1
2
k
(2) Let a 1 , a 2 ,..., anda n form a basis for V *. If 1 £ k £ n, then the set of all
aa
ŸŸŸ
...
a
,
1
£<<<£
i
i
...
i
n
,
i
i
i
12
k
1
2
k
n
k
Ê
Ë
ˆ
¯
is a basis for L k ( V ). It follows that L k ( V ) has dimension
.
(3) If a i Œ V *, then the element a 1 Ÿa 2 Ÿ ...Ÿa k ŒL k ( V ) satisfies
(
)(
) =
(
()
)
aa
ŸŸŸ
...
a
vv
,
,...,
v
det
a
v
(4.25d)
1
2
k
1
2
k
i
j
for all v j ΠV .
(4) If T : V Æ W is a linear transformation, then the induced map T* : W * Æ V *
on dual spaces defines an induced map
k
() Æ
k
()
T
*:
L
WV
,
(4.25e)
satisfying
( (
) =
(
()( )
( )
)
k
() Œ
T
*
a
vv
,
,...,
v
a
T
v
,
T
v
,...,
T
v
,
a
Œ
L
Wv V
,
(4.25f)
12
k
1
2
k
i
(
) =
() Ÿ
()
r
() Œ
s
()
T
*
ab
Ÿ
T
*
a
T
*
ba
,
Œ
L
WW
,
b
.
(4.25g)
We summarize a few basic consequences of the above for emphasis.
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