Green identity. With the outward unit normal, the product rule gives . Integrating over and applying the divergence theorem yields Green's first identity:
Uniqueness for nonzero mass. Suppose two real solutions have the same prescribed boundary data, and let be their difference. The spatial equation called the Klein-Gordon equation in the question is the modified Helmholtz equation, so . With , Green's first identity becomes
For identical Dirichlet boundary conditions, on ; for identical Neumann boundary conditions, there. Either makes the right-hand side zero. When is real and nonzero, both integrands on the left are nonnegative, forcing . Thus
This is the required uniqueness assertion; existence is understood for admissible smooth data on a suitable bounded region. Complex-valued solutions obey the same result by treating their real and imaginary parts separately.
Zero mass. For , the argument gives , hence on the connected region. Dirichlet boundary conditions still force , but Neumann boundary conditions leave an arbitrary additive constant:
The prescribed normal data in the zero-mass case must also satisfy , by the divergence theorem. For nonzero , that flux can instead equal .
Energy minimization. Let for the two functions in the last part. They share their boundary values, so on . Since is a harmonic function, Green's first identity gives
Expand the square in the Dirichlet energy of :
The cross term vanishes, so
Equality requires to be constant, and the shared boundary values then make it zero. This is the Dirichlet principle: among functions with fixed boundary values, the harmonic function minimizes Dirichlet energy.

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