 Solution

A pion mass gives a Yukawa potential range of order a femtometre, so meson exchange can describe the short range of the residual nuclear force. The nuclear suppression relative to a massless potential of the same coupling is only about a factor of two at one femtometre. A Higgs-mass mediator instead has a range around $10^{-18}\mathrm{m}$ and a further factor $e^{-633}$ by nuclear separations; direct Higgs exchange cannot supply an appreciable long-range nuclear binding interaction at those separations. The range comparison does not replace the spin, coupling and many-body physics of actual nuclear forces.