A Family of Nontrivial Homology Classes (part 2)
We continue investigating the differential forms we defined last time. Recall that we started with the position vector field and use the interior product to produce the
-form
on the punctured
-dimensional space
. We restrict this form to the
-dimensional sphere
and then pull back along the retraction mapping
to get the form
.
I’ve asserted that , and now we will prove it; let
be
tangent vectors at
and calculate
as asserted. Along the way we’ve used two things that might not be immediately apparent. First: the derivative works by transferring a vector from
to
and scaling down by a factor of
, which is a consequence of the linear action of
and the usual canonical identifications. Second: the volume form on
can be transferred to essentially the same form on
itself by using the canonical identification
.
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