A Feynman path integral method for evaluating the quantum delocalizati
on of atomic nuclei is combined with a scheme for calculating electron
ic delocalization parameters in the correlated electronic ground state
. As model system we have selected the cyclobutadiene molecule whose p
i-electronic structure is discussed in the Pariser-Parr-Pople and Hubb
ard approaches. The dynamics of the electrons are described by the cha
rge fluctuations as well as by the probabilities P(n) of finding n = 0
, 1,2 pi-electrons at the respective atomic site. For both Hamiltonian
s we have compared the pi-electron delocalization properties in the fe
rmionic state \psi(fe)] with those realized in the so-called hard core
bosonic state \psi(hcb)]. The negative sign in \psi(fe)] leads to a s
uppression of the charge fluctuations in comparison to their \psi(hcb)
] value. The dynamics of the electrons are attenuated by the quantum d
elocalization of the atomic nuclei. Details of this overall effect dep
end both on the nature of the pi-Hamiltonian and on the nature of the
electronic wavefunction.