The Tangent Bundle
UPDATE: I am aware of an issue in this post regarding the definition of the topology on the tangent bundle, namely that it is not Hausdorff and thus the tangent bundle as I've defined it is not even a topological manifold. I will correct this issue when I have time. However, the intuition and most of the details of this post are still valid, so I encourage you to read it anyway even before I correct my mistake.
Before we begin, I need to introduce a few new concepts. The first is that of a module, which is like a vector space but whose scalars come from a ring instead of a field. I guess I should formally define what a ring is before defining a module.
Definition. A ring is a set
of elements called scalars, together with two binary operations: Addition
which assigns to any pair of scalarsthe scalar , Multiplication
which assigns to any pair of scalarsthe scalar . Any ring and its operations must satisfy the following properties:
Additive Identity
There existssuch that for every . Additive Inverses
For every, there exists for which . Commutative Property of Addition
For all, we have that . Associative Property of Addition
For all, we have that . Associative Property of Multiplication
For all, we have that . Distributive Property
For all, we have that .
So basically a ring is just like a field, except it does not necessarily have a multiplicative identity or multiplicative inverses, and multiplication is not necessarily commutative. If a ring does have a multiplicative identity, it is called a ring with unity. If it additionally has multiplicative inverses (since this would make no sense without an identity) it is called a division ring. If its multiplication is commutative, it is called a commutative ring.
The definition of a module is exactly the same as that of a vector space, except its scalars come from a ring.
Definition. A module over a ring
is a set , together with two operations: Addition
which assigns to any pairthe element , Scalar Multiplication
which assigns to any scalarand any the element . Any module and its operations must satisfy the following properties:
Zero Element
There existssuch that for every . Additive Inverses
For every, there exists for which . Commutative Property of Addition
For all, we have that . Associative Property of Addition
For all, we have that . Compatibility with Ring Multiplication
For alland , we have that . Scalar Multiplicative Identity
For every, we have that . First Distributive Property
For alland , we have that . Second Distributive Property
For alland , we have that .
The next new concept we need is that of the disjoint union of sets:
Definition. Given an indexing set
and a collection of sets indexed by , their disjoint union is the set
The main point of the disjoint union is to keep an identifier for which set the elements originally came from.
Example. Let
. Normally the union of and would just be itself, since every element of is already in . However, their disjoint union is the set
Each element of this disjoint union is either of the form
or , where , so these elements look and feel just like real numbers except that we can tell whether they came from the set or .
There is, of course, no reason why all the sets being unioned together need to be the same set. Later we shall see an example where each set is different, but it is still useful to keep the identifying index.
Lastly, we will need the idea of a section. This is sort of the dual concept to that of a retraction, which I introduced when discussing the Brouwer Fixed Point Theorem in my post on connectedness.
Definition. Let
be a function between sets. A function is called a section of if . That is, if for every .
Informally speaking, sections provide a way to pick out representatives of level sets of the function
Example. Let
denote a set of people and let denote a set of continents. Define as the function which tells you which continent a person was born in. For instance, me North America.
In order to define a section
for which is the identity map on , all we need to do is send each continent to one person who lives there. Here are two possible sections for , .
Check for yourself that
and are both the identity on . And notice that my claim earlier holds true: these sections pick one representative of each continent. This concept will be very important later on.
Now we have the necessary machinery to proceed!
So far we've seen how to construct tangent vectors to a manifold at a point, and tangent spaces to manifolds at a point. But what if we wanted to do this at every point on our manifold? In multivariable calculus, we have the concept of a smooth vector field, which is an assignment of a vector to each point in
The first and most obvious problem is that defining smoothness of vector fields is going to be extremely tricky, since smoothness is a property of maps from smooth manifolds to smooth manifolds.
The second problem is even more troubling. We would like to define a vector field
So before we can proceed, we need to come up with a set comprised of all possible tangent vectors to all the points on our manifold, so this set can act as the codomain of a vector field. Furthermore, since we want a concept of smoothness for our vector fields, this set will have to be a smooth manifold. This smooth manifold I'm describing will be the tangent bundle.
Definition. Given a smooth manifold
, its tangent bundle is the set
The name "bundle" is actually very appropriate since the tangent bundle, as a set, is really just all the tangent spaces bundled together. Every element of the tangent bundle
A smooth manifold is a second countable, Hausdorff, locally Euclidean topological space. So the first thing we need to do is give
Definition. Given a smooth manifold
and its tangent bundle , the bundle projection map is the function defined by for every .
It is extremely important to note that the bundle projection map is surjective!
We will equip the tangent bundle
Let's verify that this is actually a topology, and that
Theorem. The topology on
defined above is in fact a topology, and is continuous. Proof. To show that this is a topology on the tangent bundle, we must verify three things: that the empty set and
itself are open, that the union of any collection of open sets is open, and that the intersection of any finite collection of open sets is open. To see that the empty set is open in
, we note that is open because is a topological space. Thus, is open by definition. To see that is open, we note that is open in itself, and so is open by definition. Next, we argue that the union of open sets in
is open. Let be an indexing set for which is a collection of open subsets of . Then each for some open set . It follows from the properties of the preimage that
Since the union of open sets in
is open, it follows that is open in and thus is open in . Lastly, we argue that the intersection of a finite collection of open sets in
is open. Let be a collection of open subsets of . Then each for some open set . It follows from the properties of the preimage that
Since the intersection of a finite collection of open sets in
is open, it follows that is open in and thus is open in . Thus, this is indeed a topology on . It is almost trivial to show that
is continuous. Consider any open set . Then is open in by the definition of our topology! Thus, is a continuous function.
So
To this end, choose any point
We use this information to define a chart
where
Notice that
Theorem. The set
as defined above is open in the tangent bundle . That is, if is an open set in then is an open set in . Proof. We need to construct an open set
for which . It just so happens that this set is itself, since
Since
is the preimage under of an open set in , it is open in the tangent bundle .
So we've shown that
Lastly, we should show that the atlas we've exhibited on
Lemma. Suppose
and are charts on a smooth manifold of dimension with . If and is the tangent vector
with respect to the chart map
, then
with respect to the chart map
, where each component is given by
Proof. Since
is a basis for , we know there exist scalars for which
If we apply the differential of
, the cotangent vector , to both sides of the above equation, things simplify considerably. Applying it first to the right side, we obtain
Applying
to the left side, we see that
Equating the two sides, we see that
as desired.
Now that we know how tangent vectors transform under a change of basis, we can prove that the chart maps we've defined on the tangent bundle are smooth maps in the sense of multivariable calculus.
Theorem. Let
be a smooth manifold. If and are charts for with nonempty intersection, then the transition map is smooth. Proof. Choose any point
in the image of the transition map . Then
where each
is given by
and each
is given by
These components are all smooth, since the transition map
on is smooth. It follows that the transition map on is smooth, completing the proof.
We've arrived where we wanted to: the tangent bundle is a smooth manifold! We have all the machinery we need now to develop vector fields in my next post, as well as covector and tensor fields.