  We project onto the light-front the pion's Poincare'-covariant Bethe-Salpeter
wave-function, obtained using two different approximations to the kernels of
QCD's Dyson-Schwinger equations. At an hadronic scale both computed results are
concave and significantly broader than the asymptotic distribution amplitude,
\phi_\pi^{asy}(x)=6 x(1-x); e.g., the integral of \phi_\pi(x)/\phi_\pi^{asy}(x)
is 1.8 using the simplest kernel and 1.5 with the more sophisticated kernel.
Independent of the kernels, the emergent phenomenon of dynamical chiral
symmetry breaking is responsible for hardening the amplitude.
