More onO(N)-Symmetricφ36Theory

Abstract
Large-N three-dimensional (φ2)3 field theory is studied by means of a composite-field effective potential Veff(φ,χ). Veff(φ,χ) is shown to be renormalizable in each order of the 1N expansion. When we take the first two orders into account it is found that Veff(φ,χ) is unbounded below. As a result the theory lacks a strict continuum limit for nonzero φ6 coupling and large but finite N. Our results may be of relevance to tricritical phenomena.