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Jacobi Field


A Jacobi field along a geodesic is the infinitesimal variation field of a smooth variation through geodesics. It satisfies the linear differential equation

 del _(gamma^.)^2J+R(J,gamma^.)gamma^.=0,

where R is the Riemann tensor with convention R(X,Y)=del _Xdel _Y-del _Ydel _X-del _([X,Y]). A nonzero Jacobi field vanishing at two distinct times characterizes conjugate points along the geodesic. In Euclidean space, parallel coordinates give J(t)=a+tb, so no nonzero Jacobi field vanishes at two times. On the unit sphere S^n with n>=2, along a unit-speed geodesic, a normal Jacobi field is J(t)=sin(t)E(t), where E is a nonzero parallel tangent vector field perpendicular to the geodesic's velocity. It vanishes at t=0 and t=pi, giving conjugate points at distance pi.


See also

Conjugate Point, Covariant Derivative, Geodesic, Riemann Tensor

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References

Gallier, J. and Quaintance, J. Differential Geometry and Lie Groups: A Computational Perspective. Oct. 9, 2025. https://www.engineering.upenn.edu/~jean/diffgeom-spr-I.pdf.

Cite this as:

Weisstein, Eric W. "Jacobi Field." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/JacobiField.html

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