theory with strictly locaI, non-polynomial, interacting Lagrangian
:A(x)r: 2e(x) = )__, t,-----
r=O r!
so as to preserve locality at every order. ]]>
2 - Continuum (scaling) limits of lattice fields theories (triviality of lg q in d 1=y4 dimensions
3 -Results and problems near the interface between statistical mechanics and quantum field theory]]>