The electronic spectra of one-dimensional nanostructured systems are c
alculated within the pure hopping model on the tight-binding Hamiltoni
an. By means of the renormalization group Green's function method, the
dependence of the density of states on the distributions of nanoscale
d grains and the changes of values of hopping integrals in nanostructu
red systems are studied. It is found that the frequency shifts are dep
endent rather on the changes of the hopping integrals at nanoscaled gr
ains than the distribution of nanoscaled grains.