Three loop analysis of the critical O (N) models in 6-ε dimensions
By L. Fei, S. Giombi, I. Klebanov, G. Tarnopolsky. 2014
178 citations recorded by the source corpus.
We continue the study, initiated in arXiv:1404.1094, of the $O(N)$ symmetric theory of $N+1$ massless scalar fields in $6-\epsilon$ dimensions. This theory has cubic interaction terms $\frac{1}{2}g_1 \sigma (\phi^i)^2 + \frac{1}{6}g_2 \sigma^3$. We calculate the 3-loop beta functions for the two couplings and use them to determine certain operator scaling dimensions at the IR stable fixed point up to order $\epsilon^3$. We also use the beta functions to determine the corrections to the critical value of $N$ below which there is no fixed point at real couplings. The result suggests a very significant reduction in the critical value as the dimension is decreased to $5$. We also study the theory with $N=1$, which has a $Z_2$ symmetry under $\phi\rightarrow -\phi$. We show that it possesses an IR stable fixed point at imaginary couplings which can be reached by flow from a nearby fixed point describing a pair of $N=0$ theories. We calculate certain operator scaling dimensions at the IR fixed point of the $N=1$ theory and suggest that, upon continuation to two dimensions, it describes a non-unitary conformal minimal model.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/000b64e13b0b2524dfc0ab47c06f28e6ab494263
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In Nuclear and High Energy Physics
Citations in the corpus
- Interpolating between a and F (2014, result): “r two solutions have asymptotics z (N) = p 5=N+ O 1) and they are not IR stable for generic N. 12Higher loop corrections show that the value of this critical Nis signicantly reduced as is increased [81]. 23 sin(ˇd=2) = ˇ 2 + :::in d= 6 ). Using the large Nexpressions (4.33) for the xed point couplin”
- Bootstrapping the O(N) archipelago (2015, unknown): “in other dimensions (such as in 5d [22, 28, 30, 64, 65]) may also help to shed light on these issues.”