Abstract
It is found that at available ${Q}^{2}$ the calculable perturbative contributions to the pion electric form factor ${F}_{\ensuremath{\pi}}({Q}^{2})$ and the nucleon magnetic form factors ${G}_{M}^{N}({Q}^{2})$ are much smaller than the data, which can probably be explained by soft contributions. Both hard and soft effects are estimated from light-cone/infinite-momentum-frame wave functions suggested by quark models, but the main conclusions have a more general validity.
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