We propose a method for tight-binding parametrization, designed to give acc
urate results in the calculation of confined edge states in semiconductor n
anostructures of any size. Indeed, this improved tight-binding description
accurately reproduces the bulk effective masses as well as the overall band
structure. We apply it to the specific case of silicon. The electronic sta
tes of silicon nanostructures (films, wires, and dots), with various shapes
and orientations, are calculated over large range of sizes (1-12 nm), incl
uding spin orbit. Accurate analytical laws for the confinement energies, va
lid over the whole range of sizes, are derived. Consistent comparison with
the effective mass and k.p methods show that these are only of semiquantita
tive value even for sizes as large as 8 nm. The reasons for the failure of
these techniques is analyzed in detail.