In
mathematics
Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, a vector bundle is a
topological construction that makes precise the idea of a family of
vector space
In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called ''scalars''. Scalars are often real numbers, but can ...
s parameterized by another
space
Space is the boundless three-dimensional extent in which objects and events have relative position and direction. In classical physics, physical space is often conceived in three linear dimensions, although modern physicists usually consi ...
(for example
could be a
topological space
In mathematics, a topological space is, roughly speaking, a geometrical space in which closeness is defined but cannot necessarily be measured by a numeric distance. More specifically, a topological space is a set whose elements are called poin ...
, a
manifold
In mathematics, a manifold is a topological space that locally resembles Euclidean space near each point. More precisely, an n-dimensional manifold, or ''n-manifold'' for short, is a topological space with the property that each point has a n ...
, or an
algebraic variety
Algebraic varieties are the central objects of study in algebraic geometry, a sub-field of mathematics. Classically, an algebraic variety is defined as the set of solutions of a system of polynomial equations over the real or complex numbers. ...
): to every point
of the space
we associate (or "attach") a vector space
in such a way that these vector spaces fit together to form another space of the same kind as
(e.g. a topological space, manifold, or algebraic variety), which is then called a vector bundle over
.
The simplest example is the case that the family of vector spaces is constant, i.e., there is a fixed vector space
such that
for all
in
: in this case there is a copy of
for each
in
and these copies fit together to form the vector bundle
over
. Such vector bundles are said to be
''trivial''. A more complicated (and prototypical) class of examples are the
tangent bundles of
smooth (or differentiable) manifolds: to every point of such a manifold we attach the
tangent space to the manifold at that point. Tangent bundles are not, in general, trivial bundles. For example, the tangent bundle of the sphere is non-trivial by the
hairy ball theorem. In general, a manifold is said to be
parallelizable if, and only if, its tangent bundle is trivial.
Vector bundles are almost always required to be ''locally trivial'', however, which means they are examples of
fiber bundles. Also, the vector spaces are usually required to be over the real or complex numbers, in which case the vector bundle is said to be a real or complex vector bundle (respectively).
Complex vector bundles can be viewed as real vector bundles with additional structure. In the following, we focus on real vector bundles in the
category of topological spaces.
Definition and first consequences
A real vector bundle consists of:
# topological spaces
(''base space'') and
(''total space'')
# a
continuous
Continuity or continuous may refer to:
Mathematics
* Continuity (mathematics), the opposing concept to discreteness; common examples include
** Continuous probability distribution or random variable in probability and statistics
** Continuous g ...
surjection (''bundle projection'')
# for every
in
, the structure of a
finite-dimensional
In mathematics, the dimension of a vector space ''V'' is the cardinality (i.e., the number of vectors) of a basis of ''V'' over its base field. p. 44, §2.36 It is sometimes called Hamel dimension (after Georg Hamel) or algebraic dimension to d ...
real vector space
In mathematics and physics, a vector space (also called a linear space) is a set whose elements, often called '' vectors'', may be added together and multiplied ("scaled") by numbers called ''scalars''. Scalars are often real numbers, but can ...
on the
fiber
Fiber or fibre (from la, fibra, links=no) is a natural or artificial substance that is significantly longer than it is wide. Fibers are often used in the manufacture of other materials. The strongest engineering materials often incorporate ...
where the following compatibility condition is satisfied: for every point
in
, there is an open neighborhood
of
, a
natural number
In mathematics, the natural numbers are those numbers used for counting (as in "there are ''six'' coins on the table") and ordering (as in "this is the ''third'' largest city in the country").
Numbers used for counting are called '' cardinal ...
, and a
homeomorphism
In the mathematical field of topology, a homeomorphism, topological isomorphism, or bicontinuous function is a bijective and continuous function between topological spaces that has a continuous inverse function. Homeomorphisms are the isom ...
:
such that for all
in
,
*
for all vectors
in
, and
* the map
is a linear isomorphism between the vector spaces
and
.
The open neighborhood
together with the homeomorphism
is called a local trivialization of the vector bundle. The local trivialization shows that ''locally'' the map
"looks like" the projection of
on
.
Every fiber
is a finite-dimensional real vector space and hence has a dimension
. The local trivializations show that the
function is
locally constant, and is therefore constant on each
connected component of
. If
is equal to a constant
on all of
, then
is called the rank of the vector bundle, and
is said to be a vector bundle of rank
. Often the definition of a vector bundle includes that the rank is well defined, so that
is constant. Vector bundles of rank 1 are called
line bundles, while those of rank 2 are less commonly called plane bundles.
The
Cartesian product
In mathematics, specifically set theory, the Cartesian product of two sets ''A'' and ''B'', denoted ''A''×''B'', is the set of all ordered pairs where ''a'' is in ''A'' and ''b'' is in ''B''. In terms of set-builder notation, that is
: A\t ...
, equipped with the projection
, is called the trivial bundle of rank
over
.
Transition functions
Given a vector bundle
of rank
, and a pair of neighborhoods
and
over which the bundle trivializes via
:
the composite function
:
is well-defined on the overlap, and satisfies
:
for some
-valued function
:
These are called the transition functions (or the coordinate transformations) of the vector bundle.
The set of transition functions forms a
Čech cocycle in the sense that
:
for all
over which the bundle trivializes satisfying
. Thus the data
defines a
fiber bundle; the additional data of the
specifies a
structure group in which the action on the fiber is the standard action of
.
Conversely, given a fiber bundle
with a
cocycle acting in the standard way on the fiber
, there is associated a vector bundle. This is an example of the
fibre bundle construction theorem
In mathematics, the fiber bundle construction theorem is a theorem which constructs a fiber bundle from a given base space, fiber and a suitable set of transition functions. The theorem also gives conditions under which two such bundles are isomor ...
for vector bundles, and can be taken as an alternative definition of a vector bundle.
Subbundles
One simple method of constructing vector bundles is by taking subbundles of other vector bundles. Given a vector bundle
over a topological space, a subbundle is simply a subspace
for which the restriction
of
to
gives
the structure of a vector bundle also. In this case the fibre
is a vector subspace for every
.
A subbundle of a trivial bundle need not be trivial, and indeed every real vector bundle can be viewed as a subbundle of a trivial bundle of sufficiently high rank. For example the
Möbius band
Moebius, Möbius or Mobius may refer to:
People
* August Ferdinand Möbius (1790–1868), German mathematician and astronomer
* Theodor Möbius (1821–1890), German philologist
* Karl Möbius (1825–1908), German zoologist and ecologist
* Pau ...
, a non-trivial
line bundle over the circle, can be seen as a subbundle of the trivial rank 2 bundle over the circle.
Vector bundle morphisms
A
morphism from the vector bundle
1: ''E''
1 → ''X''
1 to the vector bundle
2: ''E''
2 → ''X''
2 is given by a pair of continuous maps ''f'': ''E''
1 → ''E''
2 and ''g'': ''X''
1 → ''X''
2 such that
: ''g'' ∘
1 =
2 ∘ ''f''
::
: for every ''x'' in ''X''
1, the map
1−1() →
2−1() induced by ''f'' is a
linear map
In mathematics, and more specifically in linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is a mapping V \to W between two vector spaces that ...
between vector spaces.
Note that ''g'' is determined by ''f'' (because
1 is surjective), and ''f'' is then said to cover ''g''.
The class of all vector bundles together with bundle morphisms forms a
category. Restricting to vector bundles for which the spaces are manifolds (and the bundle projections are smooth maps) and smooth bundle morphisms we obtain the category of smooth vector bundles. Vector bundle morphisms are a special case of the notion of a
bundle map between
fiber bundles, and are sometimes called (vector) bundle homomorphisms.
A bundle homomorphism from ''E''
1 to ''E''
2 with an inverse which is also a bundle homomorphism (from ''E''
2 to ''E''
1) is called a (vector) bundle isomorphism, and then ''E''
1 and ''E''
2 are said to be isomorphic vector bundles. An isomorphism of a (rank ''k'') vector bundle ''E'' over ''X'' with the trivial bundle (of rank ''k'' over ''X'') is called a trivialization of ''E'', and ''E'' is then said to be trivial (or trivializable). The definition of a vector bundle shows that any vector bundle is locally trivial.
We can also consider the category of all vector bundles over a fixed base space ''X''. As morphisms in this category we take those morphisms of vector bundles whose map on the base space is the
identity map
Graph of the identity function on the real numbers
In mathematics, an identity function, also called an identity relation, identity map or identity transformation, is a function that always returns the value that was used as its argument, unc ...
on ''X''. That is, bundle morphisms for which the following diagram
commutes:
:
(Note that this category is ''not''
abelian
Abelian may refer to:
Mathematics Group theory
* Abelian group, a group in which the binary operation is commutative
** Category of abelian groups (Ab), has abelian groups as objects and group homomorphisms as morphisms
* Metabelian group, a grou ...
; the
kernel of a morphism of vector bundles is in general not a vector bundle in any natural way.)
A vector bundle morphism between vector bundles
1: ''E''
1 → ''X''
1 and
2: ''E''
2 → ''X''
2 covering a map ''g'' from ''X''
1 to ''X''
2 can also be viewed as a vector bundle morphism over ''X''
1 from ''E''
1 to the
pullback bundle ''g''*''E''
2.
Sections and locally free sheaves
Given a vector bundle : ''E'' → ''X'' and an open subset ''U'' of ''X'', we can consider
sections of on ''U'', i.e. continuous functions ''s'': ''U'' → ''E'' where the composite ∘ ''s'' is such that for all ''u'' in ''U''. Essentially, a section assigns to every point of ''U'' a vector from the attached vector space, in a continuous manner. As an example, sections of the tangent bundle of a differential manifold are nothing but
vector fields on that manifold.
Let ''F''(''U'') be the set of all sections on ''U''. ''F''(''U'') always contains at least one element, namely the zero section: the function ''s'' that maps every element ''x'' of ''U'' to the zero element of the vector space
−1(). With the pointwise addition and scalar multiplication of sections, ''F''(''U'') becomes itself a real vector space. The collection of these vector spaces is a
sheaf of vector spaces on ''X''.
If ''s'' is an element of ''F''(''U'') and α: ''U'' → R is a continuous map, then α''s'' (pointwise scalar multiplication) is in ''F''(''U''). We see that ''F''(''U'') is a
module
Module, modular and modularity may refer to the concept of modularity. They may also refer to:
Computing and engineering
* Modular design, the engineering discipline of designing complex devices using separately designed sub-components
* Modul ...
over the ring of continuous real-valued functions on ''U''. Furthermore, if O
''X'' denotes the structure sheaf of continuous real-valued functions on ''X'', then ''F'' becomes a sheaf of O
''X''-modules.
Not every sheaf of O
''X''-modules arises in this fashion from a vector bundle: only the
locally free ones do. (The reason: locally we are looking for sections of a projection ''U'' × R
''k'' → ''U''; these are precisely the continuous functions ''U'' → R
''k'', and such a function is a ''k''-tuple of continuous functions ''U'' → R.)
Even more: the category of real vector bundles on ''X'' is
equivalent to the category of locally free and finitely generated sheaves of O
''X''-modules.
So we can think of the category of real vector bundles on ''X'' as sitting inside the category of
sheaves of O''X''-modules; this latter category is abelian, so this is where we can compute kernels and cokernels of morphisms of vector bundles.
A rank ''n'' vector bundle is trivial if and only if it has ''n'' linearly independent global sections.
Operations on vector bundles
Most operations on vector spaces can be extended to vector bundles by performing the vector space operation ''fiberwise''.
For example, if ''E'' is a vector bundle over ''X'', then there is a bundle ''E*'' over ''X'', called the
dual bundle, whose fiber at ''x'' ∈ ''X'' is the
dual vector space (''E
x'')*. Formally ''E*'' can be defined as the set of pairs (''x'', φ), where ''x'' ∈ ''X'' and φ ∈ (''E''
''x'')*. The dual bundle is locally trivial because the
dual space
In mathematics, any vector space ''V'' has a corresponding dual vector space (or just dual space for short) consisting of all linear forms on ''V'', together with the vector space structure of pointwise addition and scalar multiplication by cons ...
of the inverse of a local trivialization of ''E'' is a local trivialization of ''E*'': the key point here is that the operation of taking the dual vector space is
functorial.
There are many functorial operations which can be performed on pairs of vector spaces (over the same field), and these extend straightforwardly to pairs of vector bundles ''E'', ''F'' on ''X'' (over the given field). A few examples follow.
* The Whitney sum (named for
Hassler Whitney) or direct sum bundle of ''E'' and ''F'' is a vector bundle ''E'' ⊕ ''F'' over ''X'' whose fiber over ''x'' is the
direct sum ''E
x'' ⊕ ''F
x'' of the vector spaces ''E
x'' and ''F
x''.
* The
tensor product bundle ''E'' ⊗ ''F'' is defined in a similar way, using fiberwise
tensor product
In mathematics, the tensor product V \otimes W of two vector spaces and (over the same field) is a vector space to which is associated a bilinear map V\times W \to V\otimes W that maps a pair (v,w),\ v\in V, w\in W to an element of V \otime ...
of vector spaces.
* The Hom-bundle Hom(''E'', ''F'') is a vector bundle whose fiber at ''x'' is the space of linear maps from ''E
x'' to ''F
x'' (which is often denoted Hom(''E''
''x'', ''F
x'') or ''L''(''E''
''x'', ''F''
''x'')). The Hom-bundle is so-called (and useful) because there is a bijection between vector bundle homomorphisms from ''E'' to ''F'' over ''X'' and sections of Hom(''E'', ''F'') over ''X''.
* Building on the previous example, given a section ''s'' of an endomorphism bundle Hom(''E'', ''E'') and a function ''f'': ''X'' → R, one can construct an eigenbundle by taking the fiber over a point ''x'' ∈ ''X'' to be the ''f''(''x'')-
eigenspace
In linear algebra, an eigenvector () or characteristic vector of a linear transformation is a nonzero vector that changes at most by a scalar factor when that linear transformation is applied to it. The corresponding eigenvalue, often denote ...
of the linear map ''s''(''x''): ''E''
''x'' → ''E''
''x''. Though this construction is natural, unless care is taken, the resulting object will not have local trivializations. Consider the case of ''s'' being the zero section and ''f'' having isolated zeroes. The fiber over these zeroes in the resulting "eigenbundle" will be isomorphic to the fiber over them in ''E'', while everywhere else the fiber is the trivial 0-dimensional vector space.
* The
dual vector bundle ''E*'' is the Hom bundle Hom(''E'', R × ''X'') of bundle homomorphisms of ''E'' and the trivial bundle R × ''X''. There is a canonical vector bundle isomorphism Hom(''E'', ''F'') = ''E*'' ⊗ ''F''.
Each of these operations is a particular example of a general feature of bundles: that many operations that can be performed on the category of vector spaces can also be performed on the category of vector bundles in a
functorial manner. This is made precise in the language of
smooth functor In differential topology, a branch of mathematics, a smooth functor is a type of functor defined on finite-dimensional real vector spaces. Intuitively, a smooth functor is smooth in the sense that it sends smoothly parameterized families of vector ...
s. An operation of a different nature is the
pullback bundle construction. Given a vector bundle ''E'' → ''Y'' and a continuous map ''f'': ''X'' → ''Y'' one can "pull back" ''E'' to a vector bundle ''f*E'' over ''X''. The fiber over a point ''x'' ∈ ''X'' is essentially just the fiber over ''f''(''x'') ∈ ''Y''. Hence, Whitney summing ''E'' ⊕ ''F'' can be defined as the pullback bundle of the diagonal map from ''X'' to ''X'' × ''X'' where the bundle over ''X'' × ''X'' is ''E'' × ''F''.
Remark: Let ''X'' be a compact space. Any vector bundle ''E'' over ''X'' is a direct summand of a trivial bundle; i.e., there exists a bundle ''E'' such that ''E'' ⊕ ''E'' is trivial. This fails if ''X'' is not compact: for example, the
tautological line bundle over the infinite real projective space does not have this property.
Additional structures and generalizations
Vector bundles are often given more structure. For instance, vector bundles may be equipped with a
vector bundle metric. Usually this metric is required to be
positive definite In mathematics, positive definiteness is a property of any object to which a bilinear form or a sesquilinear form may be naturally associated, which is positive-definite. See, in particular:
* Positive-definite bilinear form
* Positive-definite fu ...
, in which case each fibre of ''E'' becomes a Euclidean space. A vector bundle with a
complex structure corresponds to a
complex vector bundle, which may also be obtained by replacing real vector spaces in the definition with complex ones and requiring that all mappings be complex-linear in the fibers. More generally, one can typically understand the additional structure imposed on a vector bundle in terms of the resulting
reduction of the structure group of a bundle. Vector bundles over more general
topological fields may also be used.
If instead of a finite-dimensional vector space, if the fiber ''F'' is taken to be a
Banach space then a
Banach bundle is obtained. Specifically, one must require that the local trivializations are Banach space isomorphisms (rather than just linear isomorphisms) on each of the fibers and that, furthermore, the transitions
:
are continuous mappings of
Banach manifold
In mathematics, a Banach manifold is a manifold modeled on Banach spaces. Thus it is a topological space in which each point has a neighbourhood homeomorphic to an open set in a Banach space (a more involved and formal definition is given below) ...
s. In the corresponding theory for C
''p'' bundles, all mappings are required to be C
''p''.
Vector bundles are special
fiber bundles, those whose fibers are vector spaces and whose cocycle respects the vector space structure. More general fiber bundles can be constructed in which the fiber may have other structures; for example
sphere bundles are fibered by spheres.
Smooth vector bundles
A vector bundle (''E'', ''p'', ''M'') is smooth, if ''E'' and ''M'' are
smooth manifolds, p: ''E'' → ''M'' is a smooth map, and the local trivializations are
diffeomorphisms. Depending on the required degree of smoothness, there are different corresponding notions of
''Cp'' bundles,
infinitely differentiable ''C''
∞-bundles and
real analytic
In mathematics, an analytic function is a function that is locally given by a convergent power series. There exist both real analytic functions and complex analytic functions. Functions of each type are infinitely differentiable, but complex a ...
''C''
ω-bundles. In this section we will concentrate on ''C''
∞-bundles. The most important example of a ''C''
∞-vector bundle is the
tangent bundle (''TM'',
''TM'', ''M'') of a ''C''
∞-manifold ''M''.
A smooth vector bundle can be characterized by the fact that it admits transition functions as described above which are ''smooth'' functions on overlaps of trivializing charts ''U'' and ''V''. That is, a vector bundle ''E'' is smooth if it admits a covering by trivializing open sets such that for any two such sets ''U'' and ''V'', the transition function
:
is a smooth function into the matrix group GL(k,R), which is a
Lie group
In mathematics, a Lie group (pronounced ) is a group that is also a differentiable manifold. A manifold is a space that locally resembles Euclidean space, whereas groups define the abstract concept of a binary operation along with the addi ...
.
Similarly, if the transition functions are:
* ''C
r'' then the vector bundle is a ''C
r'' vector bundle,
* ''real analytic'' then the vector bundle is a real analytic vector bundle (this requires the matrix group to have a real analytic structure),
* ''holomorphic'' then the vector bundle is a
holomorphic vector bundle (this requires the matrix group to be a
complex Lie group
In geometry, a complex Lie group is a Lie group over the complex numbers; i.e., it is a complex-analytic manifold that is also a group in such a way G \times G \to G, (x, y) \mapsto x y^ is holomorphic. Basic examples are \operatorname_n(\mat ...
),
* ''algebraic functions'' then the vector bundle is an
algebraic vector bundle
In mathematics, especially in algebraic geometry and the theory of complex manifolds, coherent sheaves are a class of sheaves closely linked to the geometric properties of the underlying space. The definition of coherent sheaves is made with refer ...
(this requires the matrix group to be an
algebraic group).
The ''C''
∞-vector bundles (''E'', ''p'', ''M'') have a very important property not shared by more general ''C''
∞-fibre bundles. Namely, the tangent space ''T
v''(''E''
''x'') at any ''v'' ∈ ''E''
''x'' can be naturally identified with the fibre ''E''
''x'' itself. This identification is obtained through the ''vertical lift'' ''vl''
''v'': ''E
x'' → ''T''
''v''(''E''
''x''), defined as
:
The vertical lift can also be seen as a natural ''C''
∞-vector bundle isomorphism ''p*E'' → ''VE'', where (''p*E'', ''p*p'', ''E'') is the pull-back bundle of (''E'', ''p'', ''M'') over ''E'' through ''p'': ''E'' → ''M'', and ''VE'' := Ker(''p''
*) ⊂ ''TE'' is the ''vertical tangent bundle'', a natural vector subbundle of the tangent bundle (''TE'',
''TE'', ''E'') of the total space ''E''.
The total space ''E'' of any smooth vector bundle carries a natural vector field ''V''
''v'' := vl
''v''''v'', known as the ''canonical vector field''. More formally, ''V'' is a smooth section of (''TE'',
''TE'', ''E''), and it can also be defined as the infinitesimal generator of the Lie-group action
given by the fibrewise scalar multiplication. The canonical vector field ''V'' characterizes completely the smooth vector bundle structure in the following manner. As a preparation, note that when ''X'' is a smooth vector field on a smooth manifold ''M'' and ''x'' ∈ ''M'' such that ''X''
''x'' = 0, the linear mapping
:
does not depend on the choice of the linear covariant derivative ∇ on ''M''. The canonical vector field ''V'' on ''E'' satisfies the axioms
# The flow (''t'', ''v'') → Φ
''t''''V''(''v'') of ''V'' is globally defined.
# For each ''v'' ∈ ''V'' there is a unique lim
t→∞ Φ
''t''''V''(''v'') ∈ ''V''.
# ''C''
v(''V'')∘''C''
v(''V'') = ''C''
v(''V'') whenever ''V''
''v'' = 0.
# The zero set of ''V'' is a smooth submanifold of ''E'' whose codimension is equal to the rank of ''C''
v(''V'').
Conversely, if ''E'' is any smooth manifold and ''V'' is a smooth vector field on ''E'' satisfying 1–4, then there is a unique vector bundle structure on ''E'' whose canonical vector field is ''V''.
For any smooth vector bundle (''E'', ''p'', ''M'') the total space ''TE'' of its tangent bundle (''TE'',
''TE'', ''E'') has a natural
secondary vector bundle structure In mathematics, particularly differential topology, the secondary vector bundle structure
refers to the natural vector bundle structure on the total space ''TE'' of the tangent bundle of a smooth vector bundle , induced by the push-forward of th ...
(''TE'', ''p''
*, ''TM''), where ''p''
* is the push-forward of the canonical projection ''p'': ''E'' → ''M''. The vector bundle operations in this secondary vector bundle structure are the push-forwards +
*: ''T''(''E'' × ''E'') → ''TE'' and λ
*: ''TE'' → ''TE'' of the original addition +: ''E'' × ''E'' → ''E'' and scalar multiplication λ: ''E'' → ''E''.
K-theory
The K-theory group, , of a compact Hausdorff topological space is defined as the abelian group generated by isomorphism classes of
complex vector bundles modulo the relation that whenever we have an
exact sequence
:
then
:
in
topological K-theory.
KO-theory
In mathematics, topological -theory is a branch of algebraic topology. It was founded to study vector bundles on topological spaces, by means of ideas now recognised as (general) K-theory that were introduced by Alexander Grothendieck. The early ...
is a version of this construction which considers real vector bundles. K-theory with
compact supports can also be defined, as well as higher K-theory groups.
The famous
periodicity theorem of
Raoul Bott asserts that the K-theory of any space is isomorphic to that of the , the double suspension of .
In
algebraic geometry
Algebraic geometry is a branch of mathematics, classically studying zeros of multivariate polynomials. Modern algebraic geometry is based on the use of abstract algebraic techniques, mainly from commutative algebra, for solving geometrical ...
, one considers the K-theory groups consisting of
coherent sheaves on a
scheme A scheme is a systematic plan for the implementation of a certain idea.
Scheme or schemer may refer to:
Arts and entertainment
* ''The Scheme'' (TV series), a BBC Scotland documentary series
* The Scheme (band), an English pop band
* ''The Schem ...
, as well as the K-theory groups of vector bundles on the scheme with the above equivalence relation. The two constructs are the same provided that the underlying scheme is
smooth.
See also
General notions
*
Grassmannian:
classifying spaces for vector bundle, among which
projective spaces for
line bundles
*
Characteristic class
*
Splitting principle In mathematics, the splitting principle is a technique used to reduce questions about vector bundles to the case of line bundles.
In the theory of vector bundles, one often wishes to simplify computations, say of Chern classes. Often computation ...
*
Stable bundle In mathematics, a stable vector bundle is a (holomorphic or algebraic) vector bundle that is stable in the sense of geometric invariant theory. Any holomorphic vector bundle may be built from stable ones using Harder–Narasimhan filtration. Stabl ...
Topology and differential geometry
*
Gauge theory
In physics, a gauge theory is a type of field theory in which the Lagrangian (and hence the dynamics of the system itself) does not change (is invariant) under local transformations according to certain smooth families of operations ( Lie grou ...
: the general study of connections on vector bundles and principal bundles and their relations to physics.
*
Connection: the notion needed to differentiate sections of vector bundles.
Algebraic and analytic geometry
*
Algebraic vector bundle
In mathematics, especially in algebraic geometry and the theory of complex manifolds, coherent sheaves are a class of sheaves closely linked to the geometric properties of the underlying space. The definition of coherent sheaves is made with refer ...
*
Picard group
*
Holomorphic vector bundle
Notes
Sources
*.
*.
*, see section 1.5.
*.
*.
* see Ch.5
*.
External links
*
Why is it useful to study vector bundles ?on
MathOverflow
Why is it useful to classify the vector bundles of a space ?
{{Manifolds