Abstract

Abstract We investigate the relation between $S$-matrix unitarity ($SS^\dagger=1$) and renormalizability in theories with negative-norm states. The relation has been confirmed in many field theories, including gauge theories and Einstein gravity, by analyzing the unitarity bound, which follows from the $S$-matrix unitarity and the norm positivity. On the other hand, renormalizable theories with a higher-derivative kinetic term do not necessarily satisfy the unitarity bound because of the negative-norm states. In these theories it is not known whether the $S$-matrix unitarity provides a nontrivial constraint related to the renormalizability. In this paper, by relaxing the assumption of norm positivity we derive a bound on scattering amplitudes weaker than the unitarity bound, which may be used as a consistency requirement for $S$-matrix unitarity. We demonstrate in scalar field models with a higher-derivative kinetic term that the weaker bound and the renormalizability imply identical constraints.

Highlights

  • Unitarity and renormalizability are fundamental principles in quantum field theories (QFTs)

  • We can see the relation by the four-point vertex in the simple model that we introduce in Sect

  • We show the quantization for the fields ψ1, ψ2, and σ

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Summary

Introduction

Unitarity and renormalizability are fundamental principles in quantum field theories (QFTs). In the present paper we consider a scalar field model with a modified propagator as a toy model for quadratic gravity and demonstrate that S-matrix unitarity and renormalizability lead to identical constraints on this model. We introduce a scalar field model with a higher-derivative kinetic term as the simplest example of theories with negative-norm states. Due to the fourth-order derivative term in the kinetic term of the scalar field φ, its propagator is modified as ∼p−4 at UV and negative-norm (ghost) states appear. This model can be thought of as a toy model for quadratic gravity. Based on the extended PCR conditions, we introduce two marginal interaction terms

Renormalizable interaction terms
Non-renormalizable interaction terms
Weaker bound for amplitudes in higher-derivative scalar models
Renormalizable interaction term
Nonrenormalizable interaction term
Summary
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