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Basic Riemannian Geometry - Department of Mathematical ...

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for all ξ, η ∈ M m , m ∈ M. Since an isometry preserves the metric, it willpreserve anything built out <strong>of</strong> the metric such as the Levi–Civita connectionand its curvature. In particular, we haveK ◦ ˆΦ = K.It is not too difficult to show that, for our canonical examples, the group <strong>of</strong>all isometries acts transitively on G 2 (T M) so that K is constant. Thus wearrive at the following examples <strong>of</strong> manifolds <strong>of</strong> constant curvature:1. R n .2. S n (r).3. D n (ρ) with metricg ij =4δ ij(1 − |z| 2 /ρ 2 ) 2 .It can be shown that these exhaust all complete, simply-connected possibilities.3.5 Jacobi fieldsDefinition. Let γ : I → M be a unit speed geodesic. Say Y ∈ Γ(γ −1 T M)is a Jacobi field along γ if∇ 2 t Y + R(γ ′ , Y )γ ′ = 0.Once again we wheel out the existence and uniqueness theorems for ODEwhich tell us:Proposition. For Y 0 , Y 1 ∈ M γ(0) , there is a unique Jacobi field Y withY (0) = Y 0(∇ t Y )(0) = Y 1Jacobi fields are infinitesimal variations <strong>of</strong> γ through a family <strong>of</strong> geodesics.Indeed, suppose that h : I × (−ɛ, ɛ) → M is a variation <strong>of</strong> geodesics: thatis, each γ s : t → h(t, s) is a geodesic. Set γ = γ 0 and letY = ∂h∂s ∣ ∈ Γ(γ −1 T M).s=019

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