First let N(t) be a function such that $\int_0^a N(t)dt=0\ \forall a>0$, this is what I call a null function.
I must prove that, for every null function N(t), $\mathcal{L}\{N(t)\}=0$ (supposing that every null function can have a Laplace transform). I tried to prove it using the definition of the Laplace transform and partwise integration, and just want to check if something is wrong.
My attempt:
$\mathcal{L}\{N(t)\}=\lim_{b\to\infty}\int_0^b e^{-st}N(t)\,dt$
If we make $u=e^{-st}, dv=N(t)\,dt$, then $du=-se^{-st}dt, v=\int_0^b N(t)\,dt=0$. So we have:
$\mathcal{L}\{N(t)\}=\lim_{b\to\infty}[(0\cdot u)\mid_0^b - \int_0^b 0\cdot du]=\lim_{b\to\infty}[0]=0$
The Laplace transform, either unilateral or bilateral, of $f(t)=0$ is $F(s)=0$, simply because of linearity, by multiplying any known Laplace pair by the scalar $0$.