The Jacobi equation is the linearization of an Euler-Lagrange equation about a stationary path. Its solutions describe infinitesimal one-parameter families of stationary paths.
If is a nonvanishing solution of , expanding the right-hand side gives the displayed identity. Integrating expresses a scalar second variation as a square plus a boundary term. A simple zero of at a fixed endpoint causes no difficulty for Lipschitz endpoint-vanishing variations, since makes the boundary term tend to zero. This identity is the scalar form of a ground-state transform for a weighted Dirichlet energy.

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  1. Second variation
  2. Calculus of variations
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