I'm studying Laplace transformations, but I don't understand where $-\frac{1}{t}$ comes from. And what is the relationship between the corollary and the example?

2026-04-08 07:16:00.1775632560
Inverse Laplace transform of $\tan^{−1}\left(\frac{1}{s}\right)$
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Let $F(s)=\mathscr{L}\{f(t)\}(s)$. Then,
$$\begin{align} \mathscr{L}\{tf(t)\}&=\int_0^\infty f(t)\left(te^{-st}\right)\,dt\\\\ &=\int_0^\infty f(t)\left(-\frac{de^{-st}}{ds}\right)\,dt\\\\ &=-\frac{d}{ds}\left(\int_0^\infty f(t)e^{-st}\,dt\right)\\\\ &=-\frac{d}{ds}\left(F(s)\right) \tag 1 \end{align}$$
We can continue inductively to prove the "Corollary" in the OP.
For the case at hand, we have $F(s)=\arctan(1/s)$. Therefore,
$$-\frac{dF(s)}{ds}=\frac{1}{s^2+1}$$
Recognizing that $\frac{1}{s^2+1}$ is the Laplace Transform of $\sin(t)$, and using the result from $(1)$ gives
$$\mathscr{L}\{tf(t)\}=\mathscr{L}\{\sin(t)\}$$
from which we see immediately that $f(t)=\frac{\sin(t)}{t}$. And we are done!