Math 2.0

Differential geometry Definition

Parallel transport

Builds on Connection on a vector bundleCovariant derivative

Definition

Let MM be a smooth manifold, let E→ME \to M be a smooth vector bundle with a connection ∇\nabla, and let γ:[a,b]→M\gamma : [a, b] \to M be a piecewise smooth curve. Let DtD_t be the covariant derivative along γ\gamma. A section VV of EE along γ\gamma is parallel if DtV=0D_t V = 0. For each v∈Eγ(a)v \in E_{\gamma(a)} there is a unique parallel section VV along γ\gamma with V(a)=vV(a) = v. The parallel transport along γ\gamma is the map Pγ:Eγ(a)→Eγ(b),v↦V(b).P_\gamma : E_{\gamma(a)} \to E_{\gamma(b)}, \quad v \mapsto V(b).

Remarks

Existence and uniqueness hold because, in a local frame, DtV=0D_t V = 0 is a linear system of ordinary differential equations, whose solutions exist on the whole interval. PγP_\gamma is a linear isomorphism, its inverse is the transport along the reversed curve, and the transport along a concatenation is the composition. Example: for the flat connection on TℝnT\R^n, DtV=V˙D_t V = \dot V, so parallel sections are constant and PγP_\gamma is the identity of ℝn\R^n for every curve γ\gamma. Non-example of path independence: take the unit sphere S2S^2 with its Levi-Civita connection. Transport around the boundary of an octant, a geodesic triangle with three right angles, rotates tangent vectors by π/2\pi/2, the area of the octant. For the Levi-Civita connection of a Riemannian metric, PγP_\gamma is an isometry between tangent spaces. The connection is recovered by ∇γ′(0)s=ddt∣t=0Pγ∣[0,t]−1s(γ(t))\nabla_{\gamma'(0)} s = \frac{d}{dt}\big|_{t = 0} P_{\gamma|_{[0, t]}}^{-1} s(\gamma(t)).

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  1. Connection on a vector bundle concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Parallel_transport
About this page
TagP7YZFF8851
URIm2://P7YZFF8851
Kinddefinition
WritingW0 stub
MSC53C05, 53B05
DefinesParallel transport
UsesConnection on a vector bundle, Covariant derivative
Changed2 November 2026

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