For a variation with at both endpoints, the first variation is
Two applications of integration by parts remove derivatives from . The boundary terms vanish, and the fundamental lemma of the calculus of variations gives the higher-order Euler-Lagrange equation
For the stated integrand,
so the equation reduces to
The general solution of this linear ordinary differential equation is
Decay and finiteness of the integral force ; gives , and gives . Hence the unique stationary function is

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