Fiber bundle
In mathematics, and particularly topology, a fiber bundle (or, in Commonwealth English: fibre bundle) is a space that is locally a product space, but globally may have a different topological structure. Specifically, the similarity between a space and a product space is defined using a continuous surjective map, , that in small regions of E behaves just like a projection from corresponding regions of to . The map , called the projection or submersion of the bundle, is regarded as part of the structure of the bundle. The space is known as the total space of the fiber bundle, as the base space, and the fiber.
In the trivial case, is just , and the map π is just the projection from the product space to the first factor. This is called a trivial bundle. Examples of nontrivial fiber bundles include the Möbius strip and Klein bottle, as well as nontrivial covering spaces. Fiber bundles such as the tangent bundle of a manifold and more general vector bundles play an important role in differential geometry and differential topology, as do principal bundles.
Mappings between total spaces of fiber bundles that "commute" with the projection maps are known as bundle maps, and the class of fiber bundles forms a category with respect to such mappings. A bundle map from the base space itself (with the identity mapping as projection) to is called a section of . Fiber bundles can be specialized in a number of ways, the most common of which is requiring that the transition maps between the local trivial patches lie in a certain topological group, known as the structure group, acting on the fiber .
History
In topology, the terms fiber (German: Faser) and fiber space (gefaserter Raum) appeared for the first time in a paper by Herbert Seifert in 1933,[1][2] but his definitions are limited to a very special case. The main difference from the present day conception of a fiber space, however, was that for Seifert what is now called the base space (topological space) of a fiber (topological) space E was not part of the structure, but derived from it as a quotient space of E. The first definition of fiber space was given by Hassler Whitney in 1935 [3] under the name sphere space, but in 1940 Whitney changed the name to sphere bundle.[4]
The theory of fibered spaces, of which vector bundles, principal bundles, topological fibrations and fibered manifolds are a special case, is attributed to Seifert, Heinz Hopf, Jacques Feldbau,[5] Whitney, Norman Steenrod, Charles Ehresmann,[6][7][8] JeanPierre Serre,[9] and others.
Fiber bundles became their own object of study in the period 1935–1940. The first general definition appeared in the works of Whitney.[10]
Whitney came to the general definition of a fiber bundle from his study of a more particular notion of a sphere bundle,[11] that is a fiber bundle whose fiber is a sphere of arbitrary dimension.[12]
Formal definition
A fiber bundle is a structure , where , , and are topological spaces and is a continuous surjection satisfying a local triviality condition outlined below. The space is called the base space of the bundle, the total space, and the fiber. The map π is called the projection map (or bundle projection). We shall assume in what follows that the base space is connected.
We require that for every , there is an open neighborhood of (which will be called a trivializing neighborhood) such that there is a homeomorphism (where is the product space) in such a way that π agrees with the projection onto the first factor. That is, the following diagram should commute:

(1)
where is the natural projection and is a homeomorphism. The set of all is called a local trivialization of the bundle.
Thus for any , the preimage is homeomorphic to (since proj_{1}^{−1}({p}) clearly is) and is called the fiber over p. Every fiber bundle is an open map, since projections of products are open maps. Therefore carries the quotient topology determined by the map π.
A fiber bundle is often denoted

(2)
that, in analogy with a short exact sequence, indicates which space is the fiber, total space and base space, as well as the map from total to base space.
A smooth fiber bundle is a fiber bundle in the category of smooth manifolds. That is, , , and are required to be smooth manifolds and all the functions above are required to be smooth maps.
Examples
Trivial bundle
Let and let be the projection onto the first factor. Then is a fiber bundle (of ) over . Here is not just locally a product but globally one. Any such fiber bundle is called a trivial bundle. Any fiber bundle over a contractible CWcomplex is trivial.
Möbius strip
Perhaps the simplest example of a nontrivial bundle is the Möbius strip. It has the circle that runs lengthwise along the center of the strip as a base and a line segment for the fiber , so the Möbius strip is a bundle of the line segment over the circle. A neighborhood of (where ) is an arc; in the picture, this is the length of one of the squares. The preimage in the picture is a (somewhat twisted) slice of the strip four squares wide and one long.
A homeomorphism ( in the Formal Definition section) exists that maps the preimage of (the trivializing neighborhood) to a slice of a cylinder: curved, but not twisted. This pair locally trivializes the strip. The corresponding trivial bundle would be a cylinder, but the Möbius strip has an overall "twist". 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).
Klein bottle
A similar nontrivial bundle is the Klein bottle, which can be viewed as a "twisted" circle bundle over another circle. The corresponding nontwisted (trivial) bundle is the 2torus, .
Covering map
A covering space is a fiber bundle such that the bundle projection is a local homeomorphism. It follows that the fiber is a discrete space.
Vector and principal bundles
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. From any vector bundle, one can construct the frame bundle of bases, which is a principal bundle (see below).
Another special class of fiber bundles, called principal bundles, are bundles on whose fibers a free and transitive action by a group is given, so that each fiber is a principal homogeneous space. The bundle is often specified along with the group by referring to it as a principal bundle. The group is also the structure group of the bundle. Given a representation of on a vector space , a vector bundle with as a structure group may be constructed, known as the associated bundle.
Sphere bundles
A sphere bundle is a fiber bundle whose fiber is an nsphere. Given a vector bundle with a metric (such as the tangent bundle to a Riemannian manifold) one can construct the associated unit sphere bundle, for which the fiber over a point is the set of all unit vectors in . When the vector bundle in question is the tangent bundle , the unit sphere bundle is known as the unit tangent bundle.
A sphere bundle is partially characterized by its Euler class, which is a degree cohomology class in the total space of the bundle. In the case the sphere bundle is called a circle bundle and the Euler class is equal to the first Chern class, which characterizes the topology of the bundle completely. For any , given the Euler class of a bundle, one can calculate its cohomology using a long exact sequence called the Gysin sequence.
Mapping tori
If X is a topological space and is a homeomorphism then the mapping torus has a natural structure of a fiber bundle over the circle with fiber . Mapping tori of homeomorphisms of surfaces are of particular importance in 3manifold topology.
Quotient spaces
If is a topological group and is a closed subgroup, then under some circumstances, the quotient space together with the quotient map is a fiber bundle, whose fiber is the topological space . A necessary and sufficient condition for () to form a fiber bundle is that the mapping admit local crosssections (Steenrod 1951, §7).
The most general conditions under which the quotient map will admit local crosssections are not known, although if is a Lie group and a closed subgroup (and thus a Lie subgroup by Cartan's theorem), then the quotient map is a fiber bundle. One example of this is the Hopf fibration, , which is a fiber bundle over the sphere whose total space is . From the perspective of Lie groups, can be identified with the special unitary group . The abelian subgroup of diagonal matrices is isomorphic to the circle group , and the quotient is diffeomorphic to the sphere.
More generally, if is any topological group and a closed subgroup that also happens to be a Lie group, then is a fiber bundle.
Sections
A section (or cross section) of a fiber bundle is a continuous map such that for all x in B. Since bundles do not in general have globally defined sections, one of the purposes of the theory is to account for their existence. The obstruction to the existence of a section can often be measured by a cohomology class, which leads to the theory of characteristic classes in algebraic topology.
The most wellknown example is the hairy ball theorem, where the Euler class is the obstruction to the tangent bundle of the 2sphere having a nowhere vanishing section.
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 where U is an open set in B and for all x in U. If is a local trivialization chart then local sections always exist over U. Such sections are in 11 correspondence with continuous maps . Sections form a sheaf.
Structure groups and transition functions
Fiber bundles often come with a group of symmetries that describe the matching conditions between overlapping local trivialization charts. Specifically, let G be a topological group that acts continuously on the fiber space F on the left. We lose nothing if we require G to act faithfully on F so that it may be thought of as a group of homeomorphisms of F. A Gatlas for the bundle (E, B, π, F) is a set of local trivialization charts such that for any for the overlapping charts and the function
is given by
where t_{ij} : U_{i} ∩ U_{j} → G is a continuous map called a transition function. Two Gatlases are equivalent if their union is also a Gatlas. A Gbundle is a fiber bundle with an equivalence class of Gatlases. The group G is called the structure group of the bundle; the analogous term in physics is gauge group.
In the smooth category, a Gbundle 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
The third condition applies on triple overlaps U_{i} ∩ U_{j} ∩ U_{k} and is called the cocycle condition (see Čech cohomology). The importance of this is that the transition functions determine the fiber bundle (if one assumes the Čech cocycle condition).
A principal Gbundle is a Gbundle where the fiber F is a principal homogeneous space for the left action of G itself (equivalently, one can specify that the action of G on the fiber F is free and transitive, i.e. regular). In this case, it is often a matter of convenience to identify F with G and so obtain a (right) action of G on the principal bundle.
Bundle maps
It is useful to have notions of a mapping between two fiber bundles. Suppose that M and N are base spaces, and and are fiber bundles over M and N, respectively. A bundle map (or bundle morphism) consists of a pair of continuous[13] functions
such that . That is, the following diagram commutes:
For fiber bundles with structure group G and whose total spaces are (right) Gspaces (such as a principal bundle), bundle morphisms are also required to be Gequivariant on the fibers. This means that is also Gmorphism from one Gspace to another, i.e., for all and .
In case the base spaces M and N coincide, then a bundle morphism over M from the fiber bundle to is a map such that . This means that the bundle map covers the identity of M. That is, and the diagram commutes
Assume that both and are defined over the same base space M. A bundle isomorphism is a bundle map between π_{E} : E → M and π_{F} : F → M such that and such that φ is also a homeomorphism.[14]
Differentiable fiber bundles
In the category of differentiable manifolds, fiber bundles arise naturally as submersions of one manifold to another. Not every (differentiable) submersion ƒ : M → N from a differentiable manifold M to another differentiable manifold N gives rise to a differentiable fiber bundle. For one thing, the map must be surjective, and (M, N, ƒ) is called a fibered manifold. However, this necessary condition is not quite sufficient, and there are a variety of sufficient conditions in common use.
If M and N are compact and connected, then any submersion f : M → N gives rise to a fiber bundle in the sense that there is a fiber space F diffeomorphic to each of the fibers such that (E, B, π, F) = (M, N, ƒ, F) is a fiber bundle. (Surjectivity of ƒ follows by the assumptions already given in this case.) More generally, the assumption of compactness can be relaxed if the submersion ƒ : M → N is assumed to be a surjective proper map, meaning that ƒ^{−1}(K) is compact for every compact subset K of N. Another sufficient condition, due to Ehresmann (1951) , is that if ƒ : M → N is a surjective submersion with M and N differentiable manifolds such that the preimage ƒ^{−1}{x} is compact and connected for all x ∈ N, then ƒ admits a compatible fiber bundle structure (Michor 2008, §17).
Generalizations
 The notion of a bundle applies to many more categories in mathematics, at the expense of appropriately modifying the local triviality condition; cf. principal homogeneous space and torsor (algebraic geometry).
 In topology, a fibration is a mapping π : E → B that has certain homotopytheoretic properties in common with fiber bundles. Specifically, under mild technical assumptions a fiber bundle always has the homotopy lifting property or homotopy covering property (see Steenrod (1951, 11.7) for details). This is the defining property of a fibration.
 A section of a fiber bundle is a "function whose output range is continuously dependent on the input." This property is formally captured in the notion of dependent type.
See also
 Characteristic class
 Covering map
 Fibration
 Gauge theory
 Hopf bundle
 Ibundle
 Principal bundle
 Projective bundle
 Pullback bundle
 Universal bundle
 Fibered manifold
 Vector bundle
 Affine bundle
 Equivariant bundle
 Natural bundle
 Quasifibration
Notes
 Seifert, Herbert (1933). "Topologie dreidimensionaler gefaserter Räume". Acta Mathematica. 60: 147–238. doi:10.1007/bf02398271.
 "Topologie Dreidimensionaler Gefaserter Räume" on Project Euclid.
 Whitney, Hassler (1935). "Sphere spaces". Proceedings of the National Academy of Sciences of the United States of America. 21 (7): 464–468. Bibcode:1935PNAS...21..464W. doi:10.1073/pnas.21.7.464. PMC 1076627. PMID 16588001.
 Whitney, Hassler (1940). "On the theory of sphere bundles". Proceedings of the National Academy of Sciences of the United States of America. 26 (2): 148–153. Bibcode:1940PNAS...26..148W. doi:10.1073/pnas.26.2.148. PMC 1078023. PMID 16588328.
 Feldbau, Jacques (1939). "Sur la classification des espaces fibrés". Comptes rendus de l'Académie des Sciences. 208: 1621–1623.
 Ehresmann, Charles (1947). "Sur la théorie des espaces fibrés". Coll. Top. Alg. Paris. C.N.R.S.: 3–15.
 Ehresmann, Charles (1947). "Sur les espaces fibrés différentiables". Comptes rendus de l'Académie des Sciences. 224: 1611–1612.
 Ehresmann, Charles (1955). "Les prolongements d'un espace fibré différentiable". Comptes rendus de l'Académie des Sciences. 240: 1755–1757.
 Serre, JeanPierre (1951). "Homologie singulière des espaces fibrés. Applications". Annals of Mathematics. 54 (3): 425–505. doi:10.2307/1969485. JSTOR 1969485.
 See Steenrod (1951, Preface)
 In his early works, Whitney referred to the sphere bundles as the "spherespaces". See, for example:
 Whitney, Hassler (1935). "Sphere spaces". Proc. Natl. Acad. Sci. 21 (7): 462–468. Bibcode:1935PNAS...21..464W. doi:10.1073/pnas.21.7.464. PMC 1076627. PMID 16588001.
 Whitney, Hassler (1937). "Topological properties of differentiable manifolds". Bull. Amer. Math. Soc. 43 (12): 785–805. doi:10.1090/s000299041937066420.
 Whitney, Hassler (1940). "On the theory of sphere bundles" (PDF). Proc. Natl. Acad. Sci. 26 (2): 148–153. Bibcode:1940PNAS...26..148W. doi:10.1073/pnas.26.2.148. PMC 1078023. PMID 16588328.
 Depending on the category of spaces involved, the functions may be assumed to have properties other than continuity. For instance, in the category of differentiable manifolds, the functions are assumed to be smooth. In the category of algebraic varieties, they are regular morphisms.
 Or is, at least, invertible in the appropriate category; e.g., a diffeomorphism.
References
 Steenrod, Norman (1951), The Topology of Fibre Bundles, Princeton University Press, ISBN 9780691080550
 Steenrod, Norman (April 5, 1999). The Topology of Fibre Bundles. Princeton Mathematical Series. 14. Princeton, N.J.: Princeton University Press. ISBN 9780691005485. OCLC 40734875.CS1 maint: date and year (link)
 Bleecker, David (1981), Gauge Theory and Variational Principles, Reading, Mass: AddisonWesley publishing, ISBN 9780201100969
 Ehresmann, Charles. "Les connexions infinitésimales dans un espace fibré différentiable". Colloque de Topologie (Espaces fibrés), Bruxelles, 1950. Georges Thone, Liège; Masson et Cie., Paris, 1951. pp. 29–55.
 Husemoller, Dale (1994), Fibre Bundles, Springer Verlag, ISBN 9780387940878
 Michor, Peter W. (2008), Topics in Differential Geometry, Graduate Studies in Mathematics, Vol. 93, Providence: American Mathematical Society, ISBN 9780821820032
volume=
has extra text (help)  Voitsekhovskii, M.I. (2001) [1994], "Fibre space", Encyclopedia of Mathematics, EMS Press
External links
 Fiber Bundle, PlanetMath
 Rowland, Todd. "Fiber Bundle". MathWorld.
 Making John Robinson's Symbolic Sculpture `Eternity'
 Sardanashvily, Gennadi, Fibre bundles, jet manifolds and Lagrangian theory. Lectures for theoreticians, arXiv:0908.1886