The Hodge Star on Differential Forms
Let’s say that 
is an orientable Riemannian manifold. We know that this lets us define a (non-degenerate) inner product on differential forms, and of course we have a wedge product of differential forms. We have almost everything we need to define an analogue of the Hodge star on differential forms; we just need a particular top — or “volume” — form at each point.
To this end, pick one or the other orientation, and let 
be a coordinate patch such that the form 
is compatible with the chosen orientation. We’d like to use this form as our top form, but it’s heavily dependent on our choice of coordinates, so it’s very much not a geometric object — our ideal choice of a volume form will be independent of particular coordinates.
So let’s see how this form changes; if 
is another coordinate patch, we can assume that 
by restricting each patch to their common intersection. We’ve already determined that the forms differ by a factor of the Jacobian determinant:
What we want to do is multiply our form by some function that transforms the other way, so that when we put them together the product will be invariant.
Now, we already have something else floating around in our discussion: the metric tensor 
. When we pick coordinates 
we get a matrix-valued function:
and similarly with respect to the alternative coordinates 
:
So, what’s the difference between these two matrix-valued functions? We can calculate two ways:
That is, we transform the metric tensor with two copies of the inverse Jacobian matrix. Indeed, we could have come up with this on general principles, since has type 
— a tensor of type 
transforms with 
copies of the Jacobian and 
copies of the inverse Jacobian.
Anyway, now we can take the determinant of each side:
and taking square roots we find:
Thus the square root of the metric determinant is a function that transforms from one coordinate patch to the other by the inverse Jacobian determinant. And so we can define:
which does depend on the coordinate system to write down, but which is actually invariant under a change of coordinates! That is, 
on the intersection 
. Since the algebras of differential forms form a sheaf 
, we know that we can patch these 
together into a unique 
, and this is our volume form.
And now we can form the Hodge star, point by point. Given any 
-form 
we define the dual form 
to be the unique 
-form such that
for all -forms 
. Since at every point 
we have an inner product and a wedge 
, we can find a 
. Some general handwaving will suffice to show that varies smoothly from point to point.
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October 6, 2011 -
Posted by John Armstrong |
Differential Geometry, Geometry
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