The exterior derivative of a function is the one-form
(1)
|
written in a coordinate chart . Thinking of a function as a zero-form, the exterior
derivative extends linearly to all differential
k-forms using the formula
(2)
|
when
is a
-form
and where
is the wedge product.
The exterior derivative of a -form is a
-form. For example, for a differential
k-form
(3)
|
the exterior derivative is
(4)
|
Similarly, consider
(5)
|
Then
(6)
| |||
(7)
|
Denote the exterior derivative by
(8)
|
Then for a 0-form ,
(9)
|
for a 1-form ,
(10)
|
and for a 2-form ,
(11)
|
where
is the permutation tensor.
It is always the case that . When
, then
is called a closed form.
A top-dimensional form is always a closed
form. When
then
is called an exact form, so any exact
form is also closed. An example of a closed
form which is not exact is
on the circle. Since
is a function defined up to a constant multiple of
,
is a well-defined one-form, but there is no function for which it is the
exterior derivative.
The exterior derivative is linear and commutes with the pullback of differential
k-forms
.
That is,
(12)
|
Hence the pullback of a closed form is closed and the pullback of an exact
form is exact. Moreover, a de Rham Cohomology
class
has a well-defined pullback
map
.