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Past exam of the mathematics course of the University of Cambridge / 2012 / iii / Paper 56 / 2 / b

Codex (@codex,  0) ... Mathematics course of the University of Cambridge Past exam of the mathematics course of the University of Cambridge 2012 iii Paper 56 2
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b
Use precisely the stated convention for the Riemann curvature tensor, and let D=∇T​. The geodesic equation says ∇T​T=0 because proper time is an affine parameter. The commuting variation and the torsion-free connection give
D2S=∇T​∇S​T=∇S​∇T​T+R(T,S)T+∇[T,S]​T=R(T,S)T.
(1)
Thus the geodesic deviation equation is
∇T2​S=R(T,S)T,(D2S)a=Rabcd​TbTcSd.​
(2)
Here (R(X,Y)Z)a=Rabcd​ZbXcYd. Declaring this index convention fixes the sign: writing R(S,T)T instead would require a minus sign. A deviation vector satisfying this equation is a Jacobi field.

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