I have to demonstrate that a function $x(t)$ and his Hilbert's transform are orthogonal, it is said:
$$\int^{\infty}_{-\infty} x(t) \cdot \hat{x}(t) dt = 0$$
where:
$$\hat{x}(t) = x(t) \ast \frac{1}{\pi t} =\frac{1}{\pi} \int^{\infty}_{-\infty} \frac{x(s)}{t-s} ds$$
or, in the frequency domain:
$$\hat{x}(t) = \mathcal{F}^{-1} \lbrace -jX(f)sgn(f)\rbrace$$
with $\mathcal{F}^{-1}$ is the inverse Fourier transform and $sgn(f)$ is the sign of $f$
I have tried the exercise using Parseval's theorem:
$$\int^{\infty}_{-\infty} x^2(t) \cdot \hat{x}^2(t) dt = \int^{\infty}_{-\infty} |X(f) \ast \hat{X}(f)|^2 df = \int^{\infty}_{-\infty} |X(f) \ast (-jsgn(f)X(f))|^2 df =$$
$$= \int^{0}_{-\infty} |X(f) \ast jX(f)|^2 df + \int^{\infty}_{0} |X(f) \ast (-jX(f))|^2 df$$
Using properties of convoution ($ax(t) \ast y(t) = a(x(t) \ast y(t)$): $$\int^{\infty}_{-\infty} x^2(t) \cdot \hat{x}^2(t) dt = \int^{0}_{-\infty} | j(X(f) \ast X(f))|^2 df + \int^{\infty}_{0} |-j(X(f) \ast X(f))|^2 df =$$ $$=\int^{0}_{-\infty} |X(f) \ast X(f)|^2 df + \int^{\infty}_{0} |X(f) \ast X(f)|^2 df = $$ $$= -\int^{\infty}_{0} |X(f) \ast X(f)|^2 df + \int^{\infty}_{0} |X(f) \ast X(f)|^2 df = 0$$
But I don't know how to relationate both integrals. Maybe that isn't the way to demonstrate the exercise.
Thanks for your help.
$$<x, \hat{x}> = \int^{\infty}_{-\infty} x(t) \cdot \hat{x}(t) dt = \int_{-\infty}^{\infty} x(t) \int_{-\infty}^{\infty} \frac{x(s)}{t-s} ds dt = \\ \int_{-\infty}^{\infty} x(s) \int_{-\infty}^{\infty} -\frac{x(t)}{s-t} dt ds = - \int_{-\infty}^{\infty} x(s) \hat{x}(s) ds = - <x,\hat{x}> $$
So what must $<x,\hat{x}>$ be?