Abstract

We study the $O(N)^3$ symmetric quantum field theory of a bosonic tensor $\phi^{abc}$ with sextic interactions. Its large $N$ limit is dominated by a positive-definite operator, whose index structure has the topology of a prism. We present a large $N$ solution of the model using Schwinger-Dyson equations to sum the leading diagrams, finding that for $2.81 < d < 3$ and for $d<1.68$ the spectrum of bilinear operators has no complex scaling dimensions. We also develop perturbation theory in $3-\epsilon$ dimensions including eight $O(N)^3$ invariant operators necessary for the renormalizability. For sufficiently large $N$, we find a "prismatic" fixed point of the renormalization group, where all eight coupling constants are real. The large $N$ limit of the resulting $\epsilon$ expansions of various operator dimensions agrees with the Schwinger-Dyson equations. Furthermore, the $\epsilon$ expansion allows us to calculate the $1/N$ corrections to operator dimensions. The prismatic fixed point in $3-\epsilon$ dimensions survives down to $N\approx 53.65$, where it merges with another fixed point and becomes complex. We also discuss the $d=1$ model where our approach gives a slightly negative scaling dimension for $\phi$, while the spectrum of bilinear operators is free of complex dimensions.

Highlights

  • In recent literature, there has been considerable interest in models where the degrees of freedom transform as tensors of rank 3 or higher

  • Even if we ignore this and consider the large N limit formally, we find that in d < 4 the OðNÞ3 invariant operator φabcφabc has a complex dimension of the form d 2 þ iαðdÞ

  • Þ g1 φ φ a1b1c1 a1b2c2 φ φ a2b1c2 a3b3c1 φa3b2c3 φa2b3c3 6!. This quantum field theory (QFT) is super-renormalizable in d < 3

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Summary

INTRODUCTION

There has been considerable interest in models where the degrees of freedom transform as tensors of rank 3 or higher. We study the OðNÞ3 symmetric theory of scalar fields φabc with a sixth-order interaction, whose This QFT is super-renormalizable in d < 3. II and III, we will show that there is a smooth large N limit where g1N3 is held fixed and derive formulas for various operator dimensions in continuous d We will call this large N limit the “prismatic” limit: the leading Feynman diagrams are not the same as the melonic diagrams, which appear in the OðNÞ5 symmetric φ6 QFT for a tensor φabcde [15]. For N > Ncrit, where Ncrit ≈ 53.65, we find a prismatic RG fixed point where all eight coupling constants are real At this fixed point, ε expansions of various operator dimensions agree in the large N limit with those obtained using the Schwinger-Dyson equations. Our large N solution gives a slightly negative scaling dimension, Δφ ≈ −0.09, while the spectrum of bilinear operators is free of complex scaling dimensions

LARGE N LIMIT
The scaling dimension of φ
BILINEAR OPERATORS
Bilinears of type B
Mixing of bilinears of type A and C
Higher spin spectrum
BOSONIC QUANTUM MECHANICS
DISCUSSION
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