The idea behind this statement is that Gaussian noise with zero mean will in the long run spend as much time above 0 as it does below 0 in such a way that its total area contribution in an integral is zero if you integrate enough of it. The more you integrate, the surer you can be about it. The signal, which would be a constant in this example, always contributes the same amount of area per unit time in the integral. So
[tex]\frac{1}{t_0}\int \limits_{0}^{t_0} S + N\, dt[/tex]
N is the noise. S is the constant signal.
[tex]\frac{\int \limits_{0}^{t_0} S\, dt}{t_0} + \frac{\int \limits_{0}^{t_0}N\, dt}{t_0}[/tex]
The term on the right approaches zero for large t_0. The term on the left is a constant, so as t_0 approaches infinity, we get
[tex]\frac{t_0S}{t_0} = S[/tex]
Which has the best signal to noise ratio possible.So I just presented an intuitive argument for bettering the SNR. Is that for what you were looking?