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Exact Results for the Spectrum of the Ising Conformal Field Theory

Oleg Antipin, Jahmall Bersini, Jacob Hafjall, Giulia Muco, Francesco Sannino

Abstract

We develop a semiclassical framework to determine scaling dimensions of neutral composite operators in scalar conformal field theories. For the critical Ising $λφ^4$ theory in $d=4-ε$, we obtain the full spectrum of composite operators built out of $n$ fields transforming in the traceless-symmetric Lorentz representations to next-to-leading order in the double-scaling limit $n\rightarrow \infty$ and $λ\rightarrow 0$ with $λn$ fixed. At any given order the semiclassical expansion resums an infinite number of Feynman diagrams. Combining our results with existing perturbative computations further yields the complete five-loop scaling dimensions in the $ε$-expansion for the family of $φ^n$ operators. Finally, in three dimensions the next-to-leading order semiclassical results supersede any other existing methodology for $n \gtrsim \mathcal{O}(10)$.

Exact Results for the Spectrum of the Ising Conformal Field Theory

Abstract

We develop a semiclassical framework to determine scaling dimensions of neutral composite operators in scalar conformal field theories. For the critical Ising theory in , we obtain the full spectrum of composite operators built out of fields transforming in the traceless-symmetric Lorentz representations to next-to-leading order in the double-scaling limit and with fixed. At any given order the semiclassical expansion resums an infinite number of Feynman diagrams. Combining our results with existing perturbative computations further yields the complete five-loop scaling dimensions in the -expansion for the family of operators. Finally, in three dimensions the next-to-leading order semiclassical results supersede any other existing methodology for .

Paper Structure

This paper contains 26 equations, 2 figures, 1 table.

Figures (2)

  • Figure 1: Comparison of the band structure of the Lamé operator $L_2$ (allowed bands colored in light blue) and $\Lambda_\ell$ for $\ell=0,1,2,5,10$ (dashed lines) as a function of $m$. Complex stability angles arise when $\Lambda_\ell$ takes values inside the forbidden zones i.e., when dashed lines are inside the uncolored zones.
  • Figure 2: Solid lines: Relative difference for $\Delta_n$ (in $\%$) between the bootstrap Simmons-Duffin:2016wlqHenriksson:2022gpa and the $\epsilon$-expansion truncated to various loop orders. Dashed lines: same quantity evaluated for the corresponding Padé approximants.