ABSTRACT
The idea of running coupling constants and renormalization-group flows gives us a new language with which to discuss the qualitative behavior of scalar field theory. In our first discussion of 0 4 theory, each value of the coupling constant-and, more generally, each form of the potential and each spacetime dimension-gave a separate problem to be explored. But in Chapter 12, we saw that <fi4 theories with different values of the coupling are connected by renormalization-group flows, and that the pattern of these flows changes continuously with the spacetime dimension. In this context, it makes sense to ask the very general question: How does (j)4 theory behave as a function of the dimension? This chapter will give a detailed answer to this question.
