Away from , a Green function for this second-derivative operator is linear in . The left boundary condition makes it on , and the right Neumann boundary condition makes it constant on . Continuity gives . Integrating the distributional equation through the Dirac delta function gives the jump , so . Therefore
Apply the Green function to the forcing:
Evaluation yields
Indeed , so , and . A difference of two solutions is linear with these homogeneous boundary conditions, hence zero; the boundary value problem has a unique solution.

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