From the partial series expansion of we derive a family of FIR filters whose transfer function is defined in eq. (3) by replacing x by in eq. (2):
From the convergence disk of the power series expansion, we deduce that the family of filters converges at low frequency (i.e. ), but we will see in the following sections that this limit is usually not a key point. The transfer functions may also be recast as a nested expression corresponding to the Horner scheme (eq. 4).