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Higher sectional curvature makes jacobi fields spread faster

Statement

Assume the inherited Axiom of Countable Choice ACω.

False claim. Suppose two unit-speed geodesics γ1,γ2 in n-dimensional Riemannian manifolds have normal Jacobi fields J1,J2 with Ji(0)=0 and equal positive initial-derivative norms, and suppose every radial sectional curvature of the first manifold is at least every radial sectional curvature of the second. Then higher curvature makes the field longer: ∣J1(t)∣≥∣J2(t)∣ at every time t in the common interval of definition.

The claim is false. On a segment [0,T] where γ1(0) has no conjugate point along γ1 in (0,T], Rauch's first comparison (Rauch comparison theorem first form) gives ∣J1(t)∣≤∣J2(t)∣ for 0≤t≤T. This reversed comparison is restricted to that segment; it is not asserted beyond the first conjugate instant of the more-curved geodesic.

Facts & Assumptions

Given: The inherited ACω of [A1] and the false claim above; the refutation uses the explicit comparison pair below.

[A1]

The countable-choice premise is the inherited ACω (The Axiom of Countable Choice (ACω)), inherited through the constant-sectional-curvature and curvature-tensor interfaces below; the parallel initial-value supplier itself is choice-free.

[F1]

Comparison sine (Comparison sine, cosine and cotangent functions, Model functions solve the constant curvature jacobi equation): for k=1 one has sn⁡1(t)=sin⁡t, sn⁡1′′+sn⁡1=0, sn⁡1(0)=0, sn⁡1′(0)=1, and sn⁡1(t)>0 for 0<t<π.

[F2]

Model geometry (Constant sectional curvature and space form, Curvature tensor of constant sectional curvature, Jacobi field): a manifold of constant sectional curvature k has R(X,Y)Z=k(g(Y,Z)X−g(X,Z)Y); the unit sphere has k=1 and Euclidean space has k=0, so on a unit-speed geodesic γ and for a parallel normal unit field ΦtE the fields Jsphere(t)=sin⁡t ΦtE,Jeuclid(t)=t ΦtE satisfy Dt2J+R(J,γ˙)γ˙=0: indeed Jsphere′′=−Jsphere=−R(Jsphere,γ˙)γ˙ on the unit sphere and Jeuclid′′=0=R(Jeuclid,γ˙)γ˙ in Euclidean space.

[F3]

Parallel transport (Existence and uniqueness of parallel sections, Levi civita parallel transport preserves lengths angles and volume): the parallel field with prescribed unit normal value exists, is unique and has constant norm 1.

[F4]

Rauch comparison, first form (Rauch comparison theorem first form): under its two hypotheses the inequality is ∣J1∣≤∣J2∣ when the first manifold is the more curved one.

[F5]

The strict sine bound (Sine is positive and cosine is strictly decreasing on (0,2), with cos 2 at most -1/3, The mean value theorem, as the case g(x)=x of Cauchy's: for f continuous on [a,b] with a<b and differentiable on (a,b) there is c∈(a,b) with f(b)−f(a)=f′(c)(b−a), Sine and cosine defined by their real power series): sin⁡0=0, cos⁡0=1 and cos⁡ is strictly decreasing on [0,2], so for 0<t≤2 the mean value theorem gives sin⁡t=cos⁡ξ⋅t< t for some ξ∈(0,t).

Refutation

Proof technique: direct: exhibit the sphere-versus-Euclidean pair, check the hypotheses of the false claim, and evaluate the asserted inequality at a single time where the reverse strict inequality holds.

1.1F1F2F3given

The witness pair. [F1, F2, F3, given] Take the unit sphere Sn with its round metric of curvature 1 and Euclidean space Rn, both of dimension n≥2. Let γ1 be a unit-speed great-circle geodesic on Sn and γ2 a unit-speed straight line in Rn; let E∈Tγi(0)Mi be a unit normal vector and ΦtE its parallel transport along γi [F3]. Restrict the witness pair to [0,1]. Put J1(t):=sn⁡1(t) ΦtE=sin⁡t ΦtE,J2(t):=t ΦtE. By [F1] and [F2] both are normal Jacobi fields with Ji(0)=0,∣DtJi(0)∣=1, so the initial data have the equal positive norm required by the false claim; and ∣J1(t)∣=sin⁡t,∣J2(t)∣=t.

2.1F1F2F4step 1.1given

The curvature hypothesis holds and the true inequality is reversed. [F1, F2, F4, step 1.1, given] Every radial sectional curvature of the unit sphere is 1, and every sectional curvature of Euclidean space is 0, by [F2]; hence every radial curvature of the first manifold is at least every radial curvature of the second. For this explicit pair, [F5] gives sin⁡t≤t on [0,1], so directly ∣J1(t)∣≤∣J2(t)∣(0≤t≤1). This calculation refutes the proposed direction without needing to apply Rauch or verify its no-conjugate hypothesis.

3.1F5step 1.1step 2.1given∎

The false claim fails at t=1. [F5, step 1.1, step 2.1, given] By [F5] with t=1≤2, sin⁡1=cos⁡ξ<1 for some ξ∈(0,1), because cos⁡ is strictly decreasing on [0,2] and cos⁡0=1. Therefore ∣J1(1)∣=sin⁡1<1=∣J2(1)∣, so the inequality ∣J1(1)∣≥∣J2(1)∣ of the false claim is violated by the displayed pair, whose data satisfy every hypothesis of the claim. Hence the claim is false; the correct statement is the opposite comparison inequality of [F4], on its no-conjugate comparison interval. Both model fields are explicit, so the inherited ACω of [A1] is not drawn on beyond its declaration.

Source locator

Datar §25.2 (printed p.185) states the lesson verbatim: "larger the curvature, smaller the Jacobi fields", and §25.3 proves the corresponding norm comparison; Eschenburg §3 (Rauch I, printed p.13) states the same direction. The refutation above uses the sphere-versus-Euclidean comparison pair, where the spherical field is sin⁡t and the Euclidean field is t.

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