  The "triviality" of $(\lambda\Phi^4)_4$ quantum field theory means that the
renormalized coupling $\lambda_R$ vanishes for infinite cutoff. That result
inherently conflicts with the usual perturbative approach, which begins by
postulating a non-zero, cutoff-independent $\lambda_R$. We show how a "trivial"
solution $\lambda_R=0$ can be compatible with the known structure of
perturbation theory to arbitrarily high orders, by a simple re-arrangement of
the expansion. The "trivial" solution reproduces the result obtained by
non-perturbative renormalization of the effective potential. The physical mass
is finite, while the renormalized coupling strength vanishes: the two are NOT
proportional. The classically scale-invariant $\lambda \Phi^4$ theory coupled
to the Standard Model predicts a 2.2 TeV Higgs, but does NOT imply strong
interactions in the scalar sector.
