Download An Introduction to Riemannian Geometry by C. E. Weatherburn PDF

By C. E. Weatherburn

The aim of this e-book is to bridge the distance among differential geometry of Euclidean area of 3 dimensions and the extra complex paintings on differential geometry of generalised house. the topic is taken care of by using the Tensor Calculus, that's linked to the names of Ricci and Levi-Civita; and the ebook offers an creation either to this calculus and to Riemannian geometry. The geometry of subspaces has been significantly simplified through use of the generalized covariant differentiation brought by way of Mayer in 1930, and effectively utilized through different mathematicians.

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For each k = 1, 2, 3 find an explicit formula for the curve γk : R → SU(2) given by γk : s → Exp(s · Zk ). 7. For each k ∈ N0 define φk : C → C and ψk : C∗ → C by φk , ψk : z → z k . For which k ∈ N0 are φk , ψk immersions, submersions or embeddings. 8. Prove that the map φ : Rm → Cm given by φ : (x1 , . . , xm ) → (eix1 , . . 9. Prove that the Hopf-map φ : S 3 → S 2 with φ : (x, y) → (2x¯ y , |x|2 − |y|2) is a submersion. CHAPTER 4 The Tangent Bundle The main aim of this chapter is to introduce the tangent bundle T M of a differentiable manifold M m .

9. Let (Wβ )β∈J be a locally finite open refinement, (Wβ , xβ ) be charts on M and (fβ )β∈J be a partition of unity such that support(fβ ) is contained in Wβ . Let , Rm be the Euclidean metric on Rm . Then for β ∈ J define gβ : C2∞ (T M) → C0∞ (T M) by gβ ( ∂ ∂xβk , ∂ ∂xβl )(p) = fβ (p) · ek , el 0 Rm Then g : C2∞ (T M) → C0∞ (T M) given by g = metric on M. 11. Let (M, g) and (N, h) be Riemannian manifolds. A map φ : (M, g) → (N, h) is said to be conformal if there exists a function λ : M → R such that eλ(p) gp (Xp , Yp ) = hφ(p) (dφp (Xp ), dφp(Yp )), for all X, Y ∈ C ∞ (T M) and p ∈ M.

14. Let G be a Lie group and , e be an inner product on the tangent space Te G at the neutral element e. Then for each x ∈ G the bilinear map gx (, ) : Tx G × Tx G → R with gx (Xx , Yx ) = dLx−1 (Xx ), dLx−1 (Yx ) e is an inner product on the tangent space Tx G. The smooth tensor field g : C2∞ (T G) → C0∞ (G) given by g : (X, Y ) → (g(X, Y ) : x → gx (Xx , Yx )) is a left invariant Riemannian metric on G. Proof. 4. We shall now equip the real projective space RP m with a Riemannian metric. 15. Let S m be the unit sphere in Rm+1 and Sym(Rm+1 ) be the linear space of symmetric real (m+1)×(m+1) matrices equipped with the metric g given by g(A, B) = trace(At · B)/8.

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