Smooth Manifolds | Mathematics
1.1 Topological Manifolds
Section titled “1.1 Topological Manifolds”An -dimensional topological manifold is a topological space that is:
- Hausdorff: distinct points have disjoint neighborhoods.
- Second countable: the topology has a countable basis.
- Locally Euclidean: every point has a neighborhood homeomorphic to an open subset of .
A homeomorphism is called a coordinate chart (or just chart), and is a coordinate neighborhood.
1.2 Smooth Manifolds and Atlases
Section titled “1.2 Smooth Manifolds and Atlases”A smooth atlas on a topological -manifold is a collection of charts such that:
- The cover .
- For every pair of overlapping charts, the transition map is a smooth diffeomorphism.
Two atlases are compatible if their union is also a smooth atlas. A smooth structure on is a maximal smooth atlas.
Example 1. with the identity chart is a smooth manifold.
Example 2. is a smooth manifold. Use stereographic projection or the hemisphere charts.
Example 3. The general linear group is an open subset of , hence a smooth manifold of dimension .
Example 4. The real projective space is a smooth manifold of dimension .
1.3 Smooth Maps and Diffeomorphisms
Section titled “1.3 Smooth Maps and Diffeomorphisms”A map between smooth manifolds is smooth if for every , there exist charts near and near with , such that is smooth as a map between open subsets of Euclidean spaces.
A diffeomorphism is a smooth bijection with smooth inverse. If and are diffeomorphic, we write .
Proposition 1.1. Diffeomorphism is an equivalence relation on the class of smooth manifolds.
1.4 Tangent Spaces and Derivatives
Section titled “1.4 Tangent Spaces and Derivatives”For a smooth manifold of dimension , the tangent space at can be defined in several equivalent ways:
Definition (Derivations). A tangent vector at is a linear map satisfying the Leibniz rule:
The space of all such derivations is , an -dimensional vector space.
Definition (Curves). A tangent vector is an equivalence class of smooth curves with , where if they have the same derivative in any chart.
In local coordinates , a basis for is given by the partial derivative operators .
The differential. For a smooth map , the pushforward or differential is defined by:
for . In coordinates, is represented by the Jacobian matrix.
1.5 The Cotangent Space
Section titled “1.5 The Cotangent Space”The cotangent space is the dual vector space to . Elements are called covectors or differential 1-forms at .
In coordinates, the basis dual to is , defined by .
The differential of a function at is the covector:
In coordinates: .
1.6 Vector Fields
Section titled “1.6 Vector Fields”A smooth vector field on assigns a tangent vector smoothly to each . In coordinates:
where are smooth functions.
Integral curves. A curve is an integral curve of if . The flow of is a one-parameter family of diffeomorphisms.
Lie bracket. The Lie bracket of two vector fields is:
In coordinates: .
1.7 Practice Problems
Section titled “1.7 Practice Problems”Problem 1. Show that is a smooth manifold by constructing an atlas with two charts.
Solution. Use stereographic projection from the north and south poles. For , . For , . The transition map is smooth on .
Problem 2. Show that is a smooth manifold.
Problem 3. Prove that the tangent bundle is itself a smooth -dimensional manifold.
1.8 Intuition: What Is a Manifold?
Section titled “1.8 Intuition: What Is a Manifold?”A manifold is a space that looks like Euclidean space when you zoom in closely enough. The surface of the Earth is a two-dimensional manifold: locally it appears flat (which is why map projections work for small regions), but globally it has a different topology (it is a sphere). The key idea is that you can cover the manifold with overlapping coordinate charts, each mapping a small patch to , and the transition maps between overlapping charts are smooth.
A smooth structure on a manifold is the collection of charts that make all transition maps smooth. This is what allows you to do calculus on manifolds: derivatives, integrals, and differential equations make sense because each chart locally looks like Euclidean space. The transition maps ensure that these local constructions are compatible across overlapping charts. Partitions of unity are the technical tool that lets you glue local constructions (like Riemannian metrics or differential forms) into global ones. Manifolds are the natural setting for general relativity (spacetime is a 4-dimensional Lorentzian manifold), gauge theory (connections on principal bundles), and many areas of modern geometry and physics.
1.9 Submanifolds
Section titled “1.9 Submanifolds”Definition. A subset is an embedded submanifold of dimension if for every , there exists a chart of such that .
Example. is an embedded submanifold of dimension .
Example. The torus is an embedded submanifold of dimension .
1.9 Partitions of Unity
Section titled “1.9 Partitions of Unity”Theorem 1.2. Every smooth manifold admits a partition of unity: a collection of smooth functions such that is locally finite, each , and .
Partitions of unity are used to construct global objects (Riemannian metrics, connections) from local data.
Problem 4. Show that is diffeomorphic to the torus embedded in .
Problem 5. Construct an atlas for and verify that the transition maps are smooth.
1.10 Common Mistakes
Section titled “1.10 Common Mistakes”Mistake 1: Confusing a chart with an atlas A chart maps a single open set to , while an atlas is a collection of charts that cover the entire manifold. A single chart is not sufficient for most manifolds (e.g., requires at least two charts). An atlas must have smooth transition maps on all overlaps.
Mistake 2: Assuming embedded submanifolds are the same as immersed submanifolds An embedded submanifold has the subspace topology, while an immersed submanifold may have a finer topology. For example, a dense line on a torus is an immersed submanifold but not embedded. The key difference is that embedded submanifolds are locally flat in the ambient manifold, while immersed submanifolds may self-intersect globally.
Mistake 3: Forgetting that partitions of unity are necessary for gluing local constructions Local objects like Riemannian metrics or differential forms can be defined on each chart, but gluing them into a global object requires a partition of unity. Without it, there is no canonical way to combine local data that agree on overlaps. Partitions of unity always exist on smooth manifolds, which is a key reason smoothness is assumed.
flowchart TD A[1_Smooth Manifolds] --> B[Key Concepts] A --> C[Core Principles] A --> D[Practical Applications] B --> E[Fundamental definitions] C --> F[Design patterns] D --> G[Real-world usage]Cross-References
Section titled “Cross-References”Differential Forms: Differential forms are sections of exterior powers of the cotangent bundle on a smooth manifold.
Riemannian Geometry: A Riemannian metric assigns an inner product to each tangent space of a smooth manifold.
Vector Fields and Flows: Vector fields assign a tangent vector to each point of a manifold and generate flows via integral curves.