Haelfix said:
Interesting problem. I thought about this for awhile, and couldn't come up with a counter in D =2. Can anyone prove this statement? Its not clear to me why it should be true, and there seems to be something interesting (maybe topological) lurking behind it.
I believe it is true because of the nature of coordinate lines and their tangents in 2D.
Firstly, assume that we can find a H in 2D that is singular. Therefore the columns of H, which we'll denote \mathbf{h}_i are linearly dependant. So there exist non zero \alpha_i such that
\Sigma \alpha_i \mathbf{h}_i = \mathbf{0}
Now by the definition
\mathbf{h}_i = \int_0^1 \frac{\partial \mathbf{g}}{\partial x_i}(t \mathbf{x}) dt
Therefore
\Sigma \alpha_i \mathbf{h}_i =\int_0^1 \Sigma \alpha_i \frac{\partial \mathbf{g}}{\partial x_i}(t \mathbf{x}) dt = \mathbf{0}
Now looking at the integral along this curve. We let
\mathbf{v}(t)=\Sigma \alpha_i \frac{\partial \mathbf{g}}{\partial x_i}(t(1,0)) = \alpha_1 \frac{\partial \mathbf{g}}{\partial x_1}(t(1,0)) + \alpha_2 \frac{\partial \mathbf{g}}{\partial x_2}(t(1,0))
And so we have
\int_0^1 \mathbf{v}(t) dt = \mathbf{0}
We cannot have \mathbf{v}=\mathbf{0}, because the jacobian is always fully ranked, and hence any linear combination of its columns cannot be zero.
So \mathbf{v}(t) is non zero everywhere, and its integral is zero. But if we let \mathbf{v}(t)=\frac{d \mathbf{z}}{dt}(t), we can see that
\int_0^1 \mathbf{v}(t) dt = \int_0^1 \frac{d \mathbf{z}}{dt}(t) dt = \mathbf{z}(1)-\mathbf{z}(0) = \mathbf{0}
Which means that \mathbf{v} is the tangent vector to some
closed curve \mathbf{z}(t)
We now make a change of variables by letting
\mathbf{x}(\mathbf{u}) = \left( \begin{array}{cc}<br />
\alpha_1 & -\alpha_2 \\<br />
\alpha_2 & \alpha_1 <br />
\end{array} \right) \mathbf{u}<br />
Then it can be shown that \mathbf{v}(t) = \frac{d \mathbf{g}}{d u_1}(t(1,0)), i.e. v is the tangent vector to the u_2=0 coordinate curve. But this means that this coordinate curve is closed. Since the mapping from u to x is a diffeomorphism, and the function g is a diffeomorphism, the function from u to g is a diffeomorphism on R^2. This means that it cannot have any closed coordinate curves. Therefore we have a contridiction, and so H must be non singular.
I hope this is OK. I'm not being especially rigorous here.
In higher dimensions, some of the \alpha_i can be zero, and hence the mapping from u to x may not be a diffeomorphism. Essentially you have some wiggle room once you move into higher dimensions.