unit 9 review
Vector bundles are fundamental structures in topology, combining geometric intuition with algebraic precision. They consist of a total space, base space, and projection map, with each fiber being a vector space of fixed dimension.
Characteristic classes are topological invariants associated with vector bundles, measuring their non-triviality. These include Stiefel-Whitney classes for real bundles, Chern classes for complex bundles, and Pontryagin classes, each providing insights into the bundle's structure and properties.
Definition and Basic Properties
- Vector bundle (E,B,π) consists of total space E, base space B, and projection map π:E→B
- Each fiber π−1(b) over a point b∈B is a vector space (real or complex) of fixed dimension n
- Locally trivial condition: each point b∈B has a neighborhood U such that π−1(U) is isomorphic to U×Rn (or U×Cn)
- Isomorphism preserves the vector space structure of the fibers
- Rank of a vector bundle is the dimension of its fibers
- Vector bundles are classified up to isomorphism by their base space, rank, and the field of their fibers (real or complex)
- Morphisms between vector bundles (E,B,π) and (E′,B′,π′) are continuous maps f:E→E′ that respect the vector space structure of the fibers and commute with the projection maps
Types of Vector Bundles
- Trivial vector bundle: B×Rn (or B×Cn) with projection onto the first factor
- Tangent bundle TM of a smooth manifold M: fibers are tangent spaces TpM at each point p∈M
- Normal bundle of a submanifold N⊂M: fibers are normal spaces to N in M at each point of N
- Cotangent bundle T∗M of a smooth manifold M: fibers are dual spaces (TpM)∗ of the tangent spaces
- Line bundle: rank 1 vector bundle
- Möbius band is a non-trivial real line bundle over the circle S1
- Principal G-bundle: fibers are copies of a Lie group G acting freely and transitively on each fiber
- Associated vector bundle: constructed from a principal G-bundle using a representation of G on a vector space
Sections and Transitions
- Section of a vector bundle (E,B,π) is a continuous map s:B→E such that π∘s=idB
- Assigns a vector in the fiber to each point of the base space
- Space of sections Γ(E) is a vector space (or module) over the ring of continuous functions on B
- Transition functions describe how the local trivializations of a vector bundle are related on overlaps
- Cocycle condition ensures consistency of the transition functions
- Transition functions determine the isomorphism class of a vector bundle
- Frames: ordered bases for the fibers that vary continuously over the base space
- Local frames correspond to local trivializations
- Connection on a vector bundle: a way to parallel transport vectors along paths in the base space
- Defined using a covariant derivative operator satisfying certain properties
Operations on Vector Bundles
- Whitney sum (direct sum) of vector bundles (E,B,π) and (E′,B,π′) over the same base space B: fiberwise direct sum of the vector spaces
- Tensor product of vector bundles (E,B,π) and (E′,B,π′) over the same base space B: fiberwise tensor product of the vector spaces
- Dual bundle E∗ of a vector bundle (E,B,π): fibers are dual spaces of the original fibers
- Pullback of a vector bundle (E,B,π) along a continuous map f:B′→B: fibers over b′∈B′ are the same as fibers over f(b′)∈B
- Restriction of a vector bundle to a subspace of the base space
- Induced bundle construction: creates a vector bundle over a quotient space using a given vector bundle and a group action compatible with the projection map
- Exterior powers and symmetric powers of vector bundles: fiberwise constructions
Characteristic Classes
- Characteristic classes are invariants associated to vector bundles, measuring their non-triviality
- Stiefel-Whitney classes wi(E)∈Hi(B;Z/2Z) for real vector bundles
- w1(E) measures orientability: vanishes if and only if E is orientable
- Whitney sum formula: w(E⊕E′)=w(E)⌣w(E′), where w(E)=1+w1(E)+w2(E)+⋯
- Chern classes ci(E)∈H2i(B;Z) for complex vector bundles
- c1(E) is the first obstruction to the existence of a nowhere-zero section
- Whitney sum formula: c(E⊕E′)=c(E)⌣c(E′), where c(E)=1+c1(E)+c2(E)+⋯
- Pontryagin classes pi(E)∈H4i(B;Z) for real vector bundles
- Defined using Chern classes of the complexification: pi(E)=(−1)ic2i(E⊗C)
- Euler class e(E)∈Hn(B;Z) for oriented real vector bundles of rank n
- Measures the obstruction to the existence of a nowhere-zero section
- Related to the Euler characteristic of the base space through the Poincaré-Hopf theorem
Examples and Applications
- Möbius band as a non-trivial line bundle over the circle
- Tangent bundle of the 2-sphere S2: non-trivial, as χ(S2)=2 by the Poincaré-Hopf theorem
- Hopf fibration: non-trivial circle bundle over the 2-sphere, with total space S3
- Classifying spaces BO(n), BU(n), BSO(n) for real, complex, and oriented real vector bundles of rank n
- Characteristic classes are pulled back from universal classes on these spaces
- Gauss-Bonnet theorem: relates the Euler characteristic of a compact oriented even-dimensional Riemannian manifold to the integral of the Pfaffian of the curvature form
- Chern-Weil theory: expresses characteristic classes in terms of the curvature of a connection on the vector bundle
- Index theory: relates analytic properties of elliptic operators on a manifold to topological invariants of the manifold and its vector bundles
- Atiyah-Singer index theorem, Riemann-Roch theorem for complex manifolds
Connections to Other Areas
- Differential geometry: vector bundles as a generalization of tangent bundles, connections, curvature
- Algebraic topology: classifying spaces, characteristic classes as cohomology classes, K-theory
- Algebraic geometry: algebraic vector bundles, Chern classes in Chow rings, Grothendieck's theory of schemes
- Mathematical physics: gauge theory, Berry phase, Dirac monopole, instantons
- Representation theory: vector bundles associated to principal bundles via representations of the structure group
- Index theory: Atiyah-Singer index theorem relates topology of vector bundles to analysis of elliptic operators
- Symplectic and contact geometry: prequantization line bundles, Maslov index
- Topological quantum field theory (TQFT): vector bundles as a source of examples and inspiration for the axioms of TQFT
Problem-Solving Techniques
- Compute characteristic classes using the axioms and properties they satisfy
- Stiefel-Whitney classes: axioms of normalization, naturality, Whitney sum formula, and vanishing on trivial bundles
- Chern classes: axioms of normalization, naturality, Whitney sum formula, and vanishing on trivial bundles
- Use the splitting principle to reduce computations for higher-rank bundles to line bundles
- Apply the Gysin sequence or Leray-Hirsch theorem to compute cohomology of the total space of a vector bundle
- Utilize classifying spaces and the universal bundle to pullback characteristic classes
- Employ obstruction theory to determine the (non-)existence of certain sections or structures on a vector bundle
- Relate characteristic classes to other invariants, such as the Euler characteristic or the index of an elliptic operator
- Use the Chern-Weil theory to express characteristic classes in terms of the curvature of a connection
- Apply the Atiyah-Singer index theorem to relate the index of an elliptic operator to topological invariants of the underlying manifold and its vector bundles