ProofComplete

Distributions and Fundamental Solutions - Key Proof

We prove that convolution with a fundamental solution provides solutions to inhomogeneous PDEs, establishing the foundation for integral representation formulas.

ProofSolution via Convolution with Fundamental Solution

Let LL be a linear differential operator with constant coefficients, and EE a fundamental solution: LE=δLE = \delta.

Claim: If fD(Rn)f \in \mathcal{D}(\mathbb{R}^n) (smooth, compactly supported), then u=Efu = E * f satisfies Lu=fLu = f.

Step 1: Convolution is Well-Defined

Since ff has compact support and EE is a distribution, the convolution EfE * f is well-defined as a distribution: Ef,ϕ=E,f~ϕ\langle E * f, \phi \rangle = \langle E, \tilde{f} * \phi \rangle where f~(x)=f(x)\tilde{f}(x) = f(-x).

Moreover, since fDf \in \mathcal{D}, the result EfE * f is actually a CC^\infty function (regularity of convolutions with smooth functions).

Step 2: Apply the Operator

We compute L(Ef)L(E * f) using the fact that differentiation commutes with convolution for distributions: L(Ef)=(LE)fL(E * f) = (LE) * f

This identity holds because: L(Ef),ϕ=Ef,Lϕ=E,f~(Lϕ)\langle L(E * f), \phi \rangle = \langle E * f, L^*\phi \rangle = \langle E, \tilde{f} * (L^*\phi) \rangle =E,L(f~ϕ)=LE,f~ϕ=(LE)f,ϕ= \langle E, L^*(\tilde{f} * \phi) \rangle = \langle LE, \tilde{f} * \phi \rangle = \langle (LE) * f, \phi \rangle

Step 3: Use LE=δLE = \delta

Since LE=δLE = \delta, we have: L(Ef)=(LE)f=δf=fL(E * f) = (LE) * f = \delta * f = f

The last equality uses the fundamental property of delta: δf=f\delta * f = f for any function or distribution.

Step 4: Verify Explicitly

To see δf=f\delta * f = f explicitly: (δf)(x)=δy,f(xy)=f(x0)=f(x)(\delta * f)(x) = \langle \delta_y, f(x - y) \rangle = f(x - 0) = f(x)

Therefore, u=Efu = E * f satisfies Lu=fLu = f.

Step 5: Extension to General ff

For fLloc1f \in L^1_{\text{loc}} or more general distributions, the convolution EfE * f may require additional care (ensuring EfE * f is defined) but the formal computation remains valid in appropriate function spaces.

Remark

This proof shows why fundamental solutions are so powerful: they convert the PDE Lu=fLu = f into the explicit formula u=Efu = E * f. The hard work is finding EE, after which solutions to inhomogeneous problems are obtained by integration (convolution).

Remark

For boundary value problems, modifications are needed: the fundamental solution on Rn\mathbb{R}^n must be adjusted to Green's function satisfying boundary conditions. The proof strategy remains similar, but boundary terms appear in the representation formula.