Abstract

We construct a theory of real scalar fields that interpolates between two different theories: a Lee-Wick theory with $N$ propagator poles, including $N-1$ Lee-Wick partners, and a nonlocal infinite-derivative theory with kinetic terms modified by an entire function of derivatives with only one propagator pole. Since the latter description arises when taking the $N\rightarrow\infty$ limit, we refer to the theory as "asymptotically nonlocal." Introducing an auxiliary-field formulation of the theory allows one to recover either the higher-derivative form (for any $N$) or the Lee-Wick form of the Lagrangian, depending on which auxiliary fields are integrated out. The effective scale that regulates quadratic divergences in the large-$N$ theory is the would-be nonlocal scale, which can be hierarchically lower than the mass of the lightest Lee-Wick resonance. We comment on the possible utility of this construction in addressing the hierarchy problem.

Highlights

  • When the Higgs boson was discovered at the Large Hadron Collider (LHC) in 2012 at a mass of 125 GeV, an immediate question was this: why is it so light compared to the Planck scale at 1019 GeV? The standard model, in its present form, does not provide a mechanism that protects the Higgs mass from picking up large radiative corrections from Planck-scale physics

  • Higher-derivative quadratic terms have received substantial attention as a means of obtaining improved ultraviolet behavior of loop amplitudes. When these terms are of finite order in the number of derivatives, as in the Lee-Wick standard model [2], additional poles in the two-point function appear that correspond to new particles; these might be expected at the TeV scale if they participate in a solution to the hierarchy problem

  • In theories with higher-derivative quadratic terms of infinite order, as in models where the □ operator appears as the argument of an entire function, there are no new particles, but there are other complications: the simplest formulation of such nonlocal theories in Minkowski spacetime violate unitarity [29,31,32,33,34], a problem related to the fact that there are directions in the complex p0 plane where loop integrands diverge

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Summary

INTRODUCTION

When the Higgs boson was discovered at the Large Hadron Collider (LHC) in 2012 at a mass of 125 GeV, an immediate question was this: why is it so light compared to the Planck scale at 1019 GeV? The standard model, in its present form, does not provide a mechanism that protects the Higgs mass from picking up large radiative corrections from Planck-scale physics. The Lee-Wick standard model [2] provides an inherent mechanism to address the hierarchy problem: supplementing the spectrum of the standard model by TeV-scale LeeWick partner particles with wrong-sign kinetic and mass terms leads to a cancellation of quadratic divergences in scalar self-energies, with the precise spectrum of Lee-Wick resonances left for experiments to determine. These models have been shown to be unitary, provided certain prescriptions are adopted in momentum space to deal with the different pole structure [3] (see [4]), are causal at the. Vand suggest that no impediments exist to generalizing this framework to Abelian gauge theories, non-Abelian gauge theories, and, in principle, the entire standard model

FRAMEWORK
LEE-WICK FORM OF THE THEORY
General structure
QUADRATIC DIVERGENCES
Partial fraction method at finite N
Exactly solvable model at infinite N
Large-N comparison
CONCLUSIONS
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