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SOME ILLUSTRATIONS TO VECTOR BUNDLES September 14, 2009 O.Knill n VECTOR BUNDLE λ U: E R -1 U π (x) μ(r,v) EU E v n R φU =(π,λU) trivialization 0 π ^ ο bundle projection zero section U M m-dim manifold some notation from Cliff Taubes notes for vector bundles Propo: The smooth m+n dimensional manifold E has -1 a vector space structure on each fibre π (p) Proof: 1) on each fiber, there is a vector space structure inherited from diffeo λ . Could depend on U however. U 2) the R action μ on each fibre is compatible with n ^ the scaling multiplication on R . The zero is o(p). n 3) linearity of any map ψ on R follows from t ψ(v)= ψ(tv). (linear algebra lemma) 4) apply 3) to -1 U to see that the vector ψ=λ U’ space structure does not depend on the chart of the atlas. ολ n Lemma: A smooth map ψ on R satisfying t ψ(v)= ψ(tv) for all t,v is linear. Proof: differentiate t ψ(v)= ψ(tv) to see that ψ(v) = ψ(tv) . v * is independent of t. Call A =ψ(0) * ψ(v) = Av This is linear and A does not depend on v Remark: not true between general vector spaces V dimensions V V W or in infinite COCYCLE CONSTRUCTION U g U’ g g U’’ M g U’,U o U,U’ U’,U’’ U ,U’’ : U’ : U’’ U’ Gl(n,R) Gl(n,R) : U’’ U Gl(n,R) U bundle transition functions g U,U’’ o g U’’,U cocycle constraint = ι Define the bundle as an equivalence relation on n the disjoint union of U x R (p,v) ~ (p’,v’) if p=p’ and v’=g U’,U (p) v Propo: The cocycle definition leads to the same vector bundle E as discussed before. Proof: Assume the cocycle condition: π( (p,v) ) = p μ(r, (p,v) ) = (p,rv) λ( (p,v) ) = v EU form an atlas of E with coordinate functions (φ ,λ ) : Ε U U U and transition functions: g m R xR (x) U,U’ n TANGENT BUNDLE M U g U’ V U’,U : U’ Gl(n,R) U defined by φ φU’ U φ (V) U ψ = φU’ U’,U φ (V) U’ g g o φ -1 U’, U U’,U o = ψ g o U,U’’ U’,U’ * g U’’,U = ι cocycle constraint by chain rule U ψ o U,U’ ψ o U’,U’’ ψ U’’,U = ι VECTOR BUNDLE EXAMPLES Trivial bundle Moebius bundle Tangent bundle Cotangent bundle Normal bundle Tautological bundle Matric cocycle bundle A trivial bundle of the torus TAUTOLOGICAL BUNDLE Tangent bundle of torus WHY VECTOR BUNDLES? “Bring Vector space back in picture” (Cliff) Construct manifolds from given manifolds Understand manifolds (i.e. find invariants by imposing more structure) Important in physics: i.e. vector fields, dynamics, geodesic flow, particle physics FIBER BUNDLE EXAMPLES Unit tangent bundle (needs a metric on each fibre) Hopf fibration Billiard phase space Frame bundles Cocycles Klein bottle (circle bundle over circle) Visualiation by Thomas Banchoff (Brown University), 1990. Povray adapted from Paul MyLander, 2008 EXPLANATIONS Dimensions-math.org