The homogeneous linear differential equation can be written in divergence form:
One integration gives . Therefore the two cases are
In each case the displayed functions have linear independence throughout the interval. Imposing both homogeneous Dirichlet boundary conditions forces : for , , and for , . This also establishes uniqueness for the inhomogeneous boundary value problem.
Choose the convention , where is the Dirac delta distribution, together with . The Green's function is continuous at and obeys
These conditions follow by integrating its differential equation across ; continuity prevents a derivative of the Dirac delta distribution. If and are homogeneous solutions satisfying the left and right boundary conditions, respectively, and is their Wronskian, then
For take and . Their Wronskian is , and hence
For take and , giving and
Both formulas satisfy the endpoint conditions, continuity, and the unit jump directly. The unique solution of the boundary value problem is
The factor in the first formula matters: this Green's function is for the original monic differential operator, with ordinary measure , rather than for the operator multiplied by .
For , split the Green's function integral at . Writing and gives
For , the two integrals are
Substitution and simplification yield
At both contributions vanish. At the bracket is . The differential operator kills and sends to , so this also verifies the inhomogeneous equation.
The exceptional integer is , because then the integrals contain . In this case
and the Green's function integral becomes
Here , and . Explicitly and . Thus both exceptional and nonexceptional formulas satisfy the required boundary conditions.

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