The function returns \(C^{(i)}\). \(C^{(i)}\) tends to increase as we move to coarser scales due to
the increasing dependence in the wavelet periodogram sequences. Since the method applies to non-dyadic structures it is reasonable to propose a general rule that will apply in most cases. To accomplish this the \(C^{(i)}\) are obtained for \(T=50,100,...,6000\). Then, for each scale \(i\) the following regression is fitted
\(C^{(i)}=c_0^{(i)}+c_1^{(i)} T+ c_2^{(i)} \frac{1}{T} + c_3^{(i)} T^2 +\varepsilon.\)
The adjusted \(R^2\) was above 90% for all the scales. Having estimated the values for \(\hat{c}_0^{(i)}, \hat{c}_1^{(i)}, \hat{c}_2^{(i)}, \hat{c}_3^{(i)}\) the values can be retrieved for any sample size \(T\).