The Unapologetic Mathematician

Mathematics for the interested outsider

Classes of Manifolds

As we discussed the dimension of a manifold yesterday, we passed by an interesting construction that we want to look at in more detail.

Let (U_1,\phi_1) and (U_2,\phi_2) be two coordinate patches on an n-manifold M. We can restrict each coordinate map to the intersection of the two patches — if the intersection is empty this is trivial, but not wrong — and get a function from one open region of \mathbb{R}^n to another. Specifically, if the coordinate patches have images V_1=\phi_1(U_1\cap U_2) and V_2=\phi_2(U_1\cap U_2), then we get a function \phi_1\circ\phi_2^{-1}:V_2\to V_1. We call this the “transition function” from one coordinate patch to another, and often write it \phi_{2,1}

So what do we know about these transition functions? Well, \phi_{2,1} is a homeomorphism from V_2 to V_1, meaning it’s continuous with a continuous inverse. But remember that V_i\subseteq\mathbb{R}^n, and we know a lot about real n-dimensional space. We know all kinds of extra structure beyond just its topology, and in particular we know what it means for a function from \mathbb{R}^n to itself to be smooth.

Now, as I’ve said before, “smooth” ends up behaving like a term of art. Really what we know is what it means for a function from \mathbb{R}^n to itself to be differentiable, and for that differential to be continuous, and for there to be a second differential, and so on. We even introduced classes of functions to describe this whole tower, where C^0 consists of continuous functions, C^1 consists of continuously differentiable functions, C^2 consists of continuously twice-differentiable functions. This pattern continuous on through C^k for continuously k-times-differentiable functions, C^\infty for functions with arbitrarily many continuous derivatives, and C^\omega for “analytic” functions which are the limits of their own Taylor series.

One case we didn’t explicitly mention is PL: the class of “piecewise linear” functions. These are continuous functions that can be defined by breaking up their domains into a finite number of chunks and giving an affine function — a linear transformation plus a constant offset vector — on each chunk so that the borders line up continuously. These functions aren’t generally differentiable, since they turn sharp corners at the boundaries of chunks, but they’re pretty nicely behaved anyway. The class PL sits between C^0 and C^1.

Anyway, for each class of functions we can define a corresponding class of manifolds. If all the transition functions between all the coordinate patches are piecewise-linear, we say that we have a “PL-manifold”. If they’re all C^1, we say that we have a C^1-manifold or a “differential manifold”. This goes up through C^k-manifolds, C^\infty-manifolds, and analytic manifolds.

In practice, “smooth” ends up meaning C^\infty, so that we can always take as many derivatives as we want, but really we rarely need more than a few. Still, we’ll say “smooth” and not worry about it. And from here on all our manifolds will be smooth unless explicitly stated otherwise.

February 25, 2011 Posted by | Differential Topology, Topology | 10 Comments