I was reading from Athanosios Papoulis' "The Fourier integral and its applications." and they referenced the bilateral Laplace transform and Fourier Transform as:
$$F(p)=\int_{-\infty}^{\infty}e^{-pt}f(t)dt$$ $$F(\omega)=\int_{-\infty}^{\infty}e^{-j\omega t}f(t)dt$$
and stability indicates that the real part of $p$ must lie between $a$ an $b$.(For stability I'm guessing?)
As per the textbook, if we take the values of $p$ to be purely real and ignore the imaginary axis, then $F(\omega)$ doesn't even exist.
logically, I can't see how that could happen. I was wondering if anyone could explain how that is so. As well as why we limit the real part of $p$.(guessing it's similar to the unit circle in Z transform).