While I finish my next post on the Dirichlet problem for the Monge-Ampere equation, I thought I could mention two neat things I have learned from reading Jerry Kazdan’s survey on Prescribing the curvature of a Riemannian manifold, a short book that I recommend strongly (its a bit out of date, but hey!, geometry has advanced quite a bit in the last couple of years!)
First, a cute solution to an easily-stated problem, as observed by Wallach and Warner in 1970
Theorem: Given a compact smooth 2-d manifold and
is a 2-form such that
, then there exists a smooth Riemannian metric
on
such that
, where
is the Gauss curvature of
and
is the area form of
.
Proof: Pick your favorite metric
on
, we will prove that the metric we are looking for is in fact conformal to
, for any smooth function
, define
. Using the well known formulas for the Gauss curvature and area form of
, one arrives at the identity

where the sub-indexes
and
refer to the object corresponding to the metric
and
, in particular,
is the Laplace operator for
. Then one wants to pick
such that

or 
but, using the metric
we can write
for some
(or equivalently, using the Hodge star operator given by
) thus the
we want is the solution of the equation

but since
we have that
thus by standard elliptic theory (or Fredholm theory, etc) there exists a smooth function
solving equation (**). Thus the metric
is the one we were looking for and the theorem is proved.
Now, an easily stated problem whose solution is not likely to be as short, and has led to a lot of research in the last 2 decades. I read about it for the first time in an interview with Louis Nirenberg, which can be found here.
Open problem: Given a two dimensional Riemannian manifold, can we embed it isometrically (even just locally) in three dimensional Euclidean space?
Recall that Gauss curvature solely determines the local geometry of a 2d manifold, so its not surprising that this problem is equivalent to the following problem involving the (…tataaaaa! ) Monge-Ampere equation:
Open problem restated: Given a
function
, find (even just locally) a function
which solves the equation

but mind you, this is not your grandpa’s Monge Ampere equation, for it is not an elliptic equation unless
is strictly positive. For general
, it is an equation that varies between hyperbolic or elliptic according to the sign of
, so you run into real problems in the set of points where
vanishes . If on the other hand
is strictly negative, Kazdan says that the equation above is solved using tools from non-linear hyperbolic equations, of which sadly I know nothing. The case
is then dealt with the techniques from the last two and the next post, which I should finish in a day or two.