In mathematics, in particular in topology, a fiber bundle is a space which locally looks like a product of two spaces but may possess a different global structure. Every fiber bundle consists of a continuous surjective map π : E → B satisfying a further condition making it locally of a particularly simple form. Locally here means locally on B: if we imagine a small creature living on B with a limited horizon, it will describe the map π as a projection map from a cartesian product onto one of its factors.

Fiber bundles play an important role in the fields of differential topology and differential geometry.

Contents

1 Formal definition 2 Examples 3 Sections 4 Structure groups and transition functions 5 See also 6 External links 7 References

Formal definition

A fiber bundle consists of the data (E, B, π, F), where E, B, and F are topological spaces and π : E → B is a continuous surjection satisfying a local triviality condition outlined below. B is called the base space of the bundle, E the total space, and F the fiber. The map π is called the projection map. We shall assume in what follows that the base space B is connected.

We require that for any x in B, there is an open neighborhood U of x such that π⁻¹(U) is homeomorphic to the product space U × F, in such a way that π carries over to the projection onto the first factor. That is, the following diagram should commute:

where proj₁ : U × F → U is the natural projection and φ : π⁻¹(U) → U × F is a homeomorphism. The set of all {(U_i, φ_i)} is called a local trivialization of the bundle.

For any x in B, the preimage π⁻¹(x) is homeomorphic to F and is called the fiber over x. A fiber bundle (E, B, π, F) is often denoted

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FiberBundle-02.png
Image:FiberBundle-02.png

to indicate a short exact sequence of spaces. Note that every fiber bundle π : E → B is an open map, since projections of products are open maps. Therefore B carries the quotient topology determined by the map π.

A smooth fiber bundle is a fiber bundle in the category of smooth manifolds. That is, E, B, and F are required to be smooth manifolds and all the functions above are required to be smooth maps. This is the most common context in which fiber bundles are studied and used.

Examples

Let E = B × F and let π : E → B be the projection onto the first factor. Then E is a fiber bundle over B. Here E is not just locally a product but globally one. Any such fiber bundle is called a trivial bundle.

Perhaps the simplest example of a nontrivial bundle is the Möbius strip. The Möbius strip has a circle for a base and a line segment for the fiber. The corresponding trivial bundle would look like a cylinder, but the Möbius strip has an overall "twist". Note that this twist is visible only globally; locally the Möbius strip and the cylinder are identical (making a single vertical cut in either gives the same space).

A similiar nontrivial bundle is the Klein bottle which can be viewed as a "twisted" circle bundle over another circle. The corresponding trivial bundle would be a torus, S¹ × S¹.

Every covering space is a fiber bundle with a discrete fiber.

A special class of fiber bundles, called vector bundles, are those whose fibers are vector spaces (to qualify as a vector bundle the structure group of the bundle—see below—must be a linear group). Important examples of vector bundles include the tangent bundle and cotangent bundle of a smooth manifold.

Another special class of fiber bundles are called principal bundles. See that article for more examples.

Sections

A section (or cross section) of a fiber bundle is a continuous map f : B → E such that π(f(x))=x for all x in B. Since bundles do not in general have sections, one of the purposes of the theory is to account for their existence. This leads to the theory of characteristic classes in algebraic topology.

Often one would like to define sections only locally (especially when global sections do not exist). A local section of a fiber bundle is a continuous map f : U → E where U is an open set in B and π(f(x))=x for all x in U. If (U, φ) is a local trivialization chart then local sections always exist over U. Such sections are in 1-1 correspondence with continuous maps U → F.

Structure groups and transition functions

Fiber bundles often come with a group of symmetries which desribe the matching conditions between overlapping local trivialization charts. Specifically, let G be a topological group which acts continuously on the fiber space F on the left. We lose nothing if we require G to act effectively on F so that it may be thought of as a group of homeomorphisms of F. A G-atlas for the bundle (E, B, π, F) is a local trivialization such that for any two overlapping charts (U_i, φ_i) and (U_j, φ_j) the function

<math>\phi_i\phi_j^{-1} : (U_i \cap U_j) \times F \to (U_i \cap U_j) \times F<math>

is given by

<math>\phi_i\phi_j^{-1}(x, \xi) = (x, t_{ij}(x)\xi)<math>

where <math>t_{ij} : U_i \cap U_j \to G<math> is a continuous map called a transition function. Two G-atlases are equivalent if their union is also a G-atlas. A G-bundle is a fiber bundle with an equivalence class of G-atlases. The group G is called the structure group of the bundle.

In the smooth category, a G-bundle is a smooth fiber bundle where G is a Lie group and the corresponding action on F is smooth and the transition functions are all smooth maps.

The transition functions t_ij satisfy the following conditions

1. <math>t_{ii}(x) = 1<math>
2. <math>t_{ij}(x) = t_{ji}(x)^{-1}<math>
3. <math>t_{ik}(x) = t_{ij}(x)t_{jk}(x)<math>

The third condition applies on triple overlaps <math>U_i \cap U_j \cap U_k<math> and is called the cocycle condition (see Čech cohomology).

A principal G-bundle is G-bundle where the fiber can be identified with G itself and where there is a right action of G on the total space which is fiber preserving.

See also

• vector bundle
• principal bundle
• fibration
• covering map
• gauge theory

External links

• PlanetMath: Fiber Bundle (http://planetmath.org/encyclopedia/FiberBundle.html)
• MathWorld: Fiber Bundle (http://mathworld.wolfram.com/FiberBundle.html)

References

• Norman Steenrod, The Topology of Fiber Bundles, Princeton University Press (1951). ISBN 0-691-00548-6.
• David Bleecker, Gauge Theory and Variational Principles, Addison-Wesley publishing, Reading, Mass (1981). ISBN 0-201-10096-7. See chapter one.

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