Fundamental Solution to Reduced Linear First Order ODE with Constant Coefficients
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Theorem
Let $H$ be the Heaviside step function.
Let $\lambda \in \R$.
Let $\map f x = \map H x \map \exp {\lambda x}$.
Let $T_f$ be the distribution associated with $f$.
Then, in the distributional sense, $T_f$ is the fundamental solution of
- $\paren {\dfrac \d {\d x} - \lambda} T_f = \delta$
Proof
$x \stackrel f {\longrightarrow} \map H x \map \exp {\lambda x}$ is a continuously differentiable real function on $\R \setminus \set 0$ and possibly has a discontinuity at $x = 0$.
By Differentiable Function as Distribution we have that $T'_f = T_{f'}$.
Moreover:
- $x < 0 \implies \paren {\map H x \map \exp {\lambda x}}' = 0$.
- $x > 0 \implies \paren {{\map H x} \map \exp { \lambda x}}' = \lambda \map \exp {\lambda x}$.
Altogether:
- $\forall x \in \R \setminus \set 0 : \paren {{\map H x} \map \sin x}' = \lambda \map H x \map \exp {\lambda x}$
Furthermore:
- $\ds \map f {0^+} - \map f {0^-} = \map H {0^+} \map \exp {0^+} - \map H {0^-} \map \exp {0^-} = 1$
By the Jump Rule:
- $T'_{\map H x \map \exp {\lambda x}} = T_{\lambda \map H x \map \exp {\lambda x}} + \delta$
Rearranging the terms and using the linearity of distribution gives:
- $T'_{\map H x \map \exp {\lambda x}} - \lambda T_{\map H x \map \exp {\lambda x}} = \delta$
$\blacksquare$
See also
Sources
- 2017: Amol Sasane: A Friendly Approach to Functional Analysis ... (previous) ... (next): Chapter $\S 6.4$: A glimpse of distribution theory. Multiplication by $C^\infty$ functions