| |
| | Renormalizable "non-renormalizable" theories |
 | | You can prove, under very general conditions, that after dumping some arbitrary mix of bosons, scalar fields and fermions (subject to the power counting criteria), and imposing a suitable gauge principle, you automatically get Yang-Mills with a Higgs sector for the resulting Lagrangian. |
 | | If the original theory was, in contract, NOT renormalizable, then the number of terms generated by the above process will be infinite and the resulting Lagrangian will be non-polynomial. |
 | | What I'm guessing is that with a suitably formulated gauge invariance principle, you can actually constrain the forms of these terms (DESPITE there being an infinite number of them) so that the resulting Lagrangian resides in only a finitely-parametrized family of functions, possibly even unique. |
| www.lns.cornell.edu /spr/2002-06/msg0042623.html (851 words) |
|