Given $G \in \mathcal{D}'(\mathbb{R})$, $n\in \mathbb{N}$ find the solution for $$\partial_x^nG=\delta$$
I know that this solution should be $$G=\frac{x^{n-1}}{(n-1)!}\Theta(x)$$ but I am struggling to find a proper derivation.
I can prove that for $n=1$ one gets $G=\Theta(x)$ but after that my approaches start to get a bit too heretic.
2026-03-25 02:59:29.1774407569
How to properly determine Green's Function for $\partial^n$?
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You can use your proof for $n=1$ as a base case for an induction proof. So in the induction step you determine the action on a test function $\phi \in \mathcal{D}(\mathbb{R})$:
\begin{align} \left\langle {\partial_x}^{n+1} \left(\frac{x^n}{n!} \Theta(x)\right), \phi\right\rangle &= (-1)^{n-1} \left\langle {\partial_x} \left(\frac{x^n}{n!} \Theta(x)\right), \partial_x \phi\right\rangle \quad \text{(derivative of distributions)} \\ &= (-1)^{n-1} \bigg[ \left\langle \frac{x^{n-1}}{(n-1)!} \Theta(x), {\partial_x}^{n-1}\phi\right\rangle \\ & \quad + \left\langle \frac{x^n}{n!}\delta, {\partial_x}^{n-1}\phi\right\rangle \bigg]~. \quad \text{(using product rule and base case)} \\ \end{align}
Now the first is exactly the action of ${\partial_x}^n(x^{n-1}/(n-1)!)$ on $\phi$ and thus equal to $\langle \delta, \phi \rangle$; the second term vanishes when you 'shift' the multiplication by $x^n/(n-1)!$ to the test function and apply the definition of the delta distribution:
$$ \left\langle \frac{x^n}{n!}\delta, {\partial_x}^{n-1}\phi\right\rangle = \left\langle \delta, \frac{x^n}{n!}{\partial_x}^{n-1}\phi\right\rangle = 0~. $$
I'm guessing you can also approach the problem using Fourier transforms to derive the expression for $G$, which might seem more direct as you don't need to know the answer beforehand.