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$O(N)$ Random Tensor Models

Sylvain Carrozza, Adrian Tanasa

TL;DR

The paper develops real tensor models with $O(N)^{\otimes3}$ invariance, showing a robust $1/N$ expansion for general interactions and focusing on a quartic model that combines tetrahedral and pillow interactions. Leading graphs are melonic, as in MO/$U(N)^{\otimes3}$ models, while next-to-leading graphs are obtained by melonic 2-point insertions into a finite set of core graphs, enabling a precise analytic combinatorics treatment. The authors derive generating functions, diagrammatic equations, and a singularity analysis that yield the critical curve $g_c(\mu)$ and establish LO and NLO critical exponents $\gamma_{LO}=1/2$ and $\gamma_{NLO}=3/2$, indicating universality with known tensor models. These results pave the way for double-scaling limits and broader explorations of tensorial group field theories in an enlarged interaction space.

Abstract

We define in this paper a class of three indices tensor models, endowed with $O(N)^{\otimes 3}$ invariance ($N$ being the size of the tensor). This allows to generate, via the usual QFT perturbative expansion, a class of Feynman tensor graphs which is strictly larger than the class of Feynman graphs of both the multi-orientable model (and hence of the colored model) and the $U(N)$ invariant models. We first exhibit the existence of a large $N$ expansion for such a model with general interactions. We then focus on the quartic model and we identify the leading and next-to-leading order (NLO) graphs of the large $N$ expansion. Finally, we prove the existence of a critical regime and we compute the critical exponents, both at leading order and at NLO. This is achieved through the use of various analytic combinatorics techniques.

$O(N)$ Random Tensor Models

TL;DR

The paper develops real tensor models with invariance, showing a robust expansion for general interactions and focusing on a quartic model that combines tetrahedral and pillow interactions. Leading graphs are melonic, as in MO/ models, while next-to-leading graphs are obtained by melonic 2-point insertions into a finite set of core graphs, enabling a precise analytic combinatorics treatment. The authors derive generating functions, diagrammatic equations, and a singularity analysis that yield the critical curve and establish LO and NLO critical exponents and , indicating universality with known tensor models. These results pave the way for double-scaling limits and broader explorations of tensorial group field theories in an enlarged interaction space.

Abstract

We define in this paper a class of three indices tensor models, endowed with invariance ( being the size of the tensor). This allows to generate, via the usual QFT perturbative expansion, a class of Feynman tensor graphs which is strictly larger than the class of Feynman graphs of both the multi-orientable model (and hence of the colored model) and the invariant models. We first exhibit the existence of a large expansion for such a model with general interactions. We then focus on the quartic model and we identify the leading and next-to-leading order (NLO) graphs of the large expansion. Finally, we prove the existence of a critical regime and we compute the critical exponents, both at leading order and at NLO. This is achieved through the use of various analytic combinatorics techniques.

Paper Structure

This paper contains 13 sections, 15 theorems, 72 equations, 14 figures.

Key Result

Proposition 1

The sets of Feynman graphs generated by the MO action or a $\mathrm{U}(N)^{\otimes 3}$ invariant action are strict subsets of the set of Feynman graphs generated by the real action action.

Figures (14)

  • Figure 1: The two- and four-valent bubbles/vertices of the model.
  • Figure 2: The unique MO interaction vertex.
  • Figure 3: A Feynman graph of the $\mathrm{O}(N)^{\otimes 3}$ model which is neither MO nor bipartite.
  • Figure 4: Two vacuum (and melonic) graphs.
  • Figure 5: Jackets associated to the tensor graphs of Figure \ref{['ex_ampl']}. On the right-hand-side, two connected components are generated by the removal of the lines of color $\ell$.
  • ...and 9 more figures

Theorems & Definitions (33)

  • Proposition 1
  • proof
  • Definition 1
  • Lemma 1
  • proof
  • Proposition 2
  • proof
  • Proposition 3
  • proof
  • Definition 2
  • ...and 23 more