The $O(N)$ Model in $4<d<6$: Instantons and Complex CFTs
Authors: Simone Giombi, Richard Huang, Igor R. Klebanov, Silviu S. Pufu, Grigory Tarnopolsky
AI-generated Key Points
- Study of the scalar $O(N)$ model in the dimension range $4<d<6"
- Previous work shows a fixed point where operator scaling dimensions are real and above unitarity bound
- Scaling dimensions acquire small imaginary parts due to instanton effects
- Imaginary parts are of order $e^{-N f(d)}$ for large $N$, where $f(d)$ is the sphere free energy of a conformal scalar in $(d-2)$ dimensions
- Implies that at large enough values of $N$, $O(N)$ models can be considered as complex CFTs in the range of $4<d<6$
- Non-perturbatively small imaginary parts also appear in other observables such as sphere free energy and two/three-point function coefficients
- Calculations related to these observables have significant implications
- Numerically negligible imaginary parts allow for studying five-dimensional O(N) models using numerical bootstrap techniques
- Provides new insights into behavior of scalar O(N) models in higher dimensions and their connection to complex CFTs
- Opens up avenues for further research and exploration in this field.
Abstract: We revisit the scalar $O(N)$ model in the dimension range $4<d<6$ and study the effects caused by its metastability. As shown in previous work, this model formally possesses a fixed point where, perturbatively in the $1/N$ expansion, the operator scaling dimensions are real and above the unitarity bound. Here, we further show that these scaling dimensions do acquire small imaginary parts due to the instanton effects. In $d$ dimensions and for large $N$, we find that they are of order $e^{-N f(d)}$, where, remarkably, the function $f(d)$ equals the sphere free energy of a conformal scalar in $d-2$ dimensions. The non-perturbatively small imaginary parts also appear in other observables, such as the sphere free energy and two and three-point function coefficients, and we present some of their calculations. Therefore, at sufficiently large $N$, the $O(N)$ models in $4<d<6$ may be thought of as complex CFTs. When $N$ is large enough for the imaginary parts to be numerically negligible, the five-dimensional $O(N)$ models may be studied using the techniques of numerical bootstrap.
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