In this paper, we resolve a long-standing open statistical problem. The problem is to mathematically confirm Yuleās1926 empirical finding of ānonsense correlationā. We do so by analytically determining the second moment [variance] of the empirical correlation coefficient:
Using tools from Fredholm integral equation theory, we successfully calculate the second moment of Īø to obtain a value for the standard deviation of Īø of nearly 0.5. The ānonsenseā correlation, which we call āvolatileā correlation, is volatile in the sense that its distribution is heavily dispersed and is frequently large in absolute value. It is induced because each Wiener process is āself-correlatedā in time. This is because a Wiener process is an integral of pure noise and thus its values at different time points are correlated.
In addition to providing an explicit formula for the second moment of Īø, we offer implicit formulas for higher moments of Īø.