We investigate the structure of the experimentally significant electro
weak bosonic loop corrections to the leptonic weak mixing angle, the l
eptonic Z-boson decay width, and the W-boson mass. It is shown that th
e bosonic corrections that have a sizable effect at the present level
of experimental accuracy are directly related to the use of the Fermi
constant G(mu) as input parameter for analyzing the LEP observables. I
ndeed, if the (theoretical value of the) leptonic width of the W boson
is used as input parameter instead of the low-energy parameter G(mu)
determined from muon decay, fermion-loop corrections are sufficient fo
r compatibility between theory and experiment.