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Calculating the partition function of N=2 Gauge theories on $S^3$ and AdS/CFT correspondence

Sangmo Cheon, Hyojoong Kim, Nakwoo Kim

TL;DR

This work tests AdS$_4$/CFT$_3$ for ${\cal N}=2$ quiver Chern-Simons-matter theories by computing the three-sphere partition function $Z$ via localization, reducing it to a matrix model, and analyzing the large-$N$ limit. Focusing on non-chiral theories dual to ${\rm AdS}_4\times X^7$ with $X^7\in\{Q^{1,1,1}, V^{5,2}\}$, the authors derive saddle-point equations for eigenvalues and obtain explicit $N^{3/2}$ scaling of the free energy $F=-\log Z$, with coefficients that match the volumes of the internal manifolds: ${\rm Vol}(Q^{1,1,1})$ and ${\rm Vol}(V^{5,2})$. Through detailed treatment of adjoint and fundamental matter in three examples, they show how marginality and $F$-extremization constrain R-charges to reproduce gravity results, providing strong evidence for the AdS$_4$/CFT$_3$ dictionary in these ${\cal N}=2$ settings. The work also highlights the tractability of non-chiral models and discusses limitations and future directions for chiral theories.

Abstract

We test the AdS/CFT correspondence by computing the partition function of some $\mathcal{N}=2$ quiver Chern-Simons-matter theories on three-sphere. The M-theory backgrounds are of the Freund-Rubin type with the seven-dimensional internal space given as Sasaki-Einstein manifolds $Q^{1,1,1}$ or $V^{5,2}$. Localization technique reduces the exact path integral to a matrix model, and we study the large-N behavior of the partition function. For simplicity we consider only non-chiral models which have a real-valued partition function. The result is in full agreement with the prediction of the gravity duals, i.e. the free energy is proportional to $N^{3/2}$ and the coefficient matches correctly the volume of $Q^{1,1,1}$ and $V^{5,2}$.

Calculating the partition function of N=2 Gauge theories on $S^3$ and AdS/CFT correspondence

TL;DR

This work tests AdS/CFT for quiver Chern-Simons-matter theories by computing the three-sphere partition function via localization, reducing it to a matrix model, and analyzing the large- limit. Focusing on non-chiral theories dual to with , the authors derive saddle-point equations for eigenvalues and obtain explicit scaling of the free energy , with coefficients that match the volumes of the internal manifolds: and . Through detailed treatment of adjoint and fundamental matter in three examples, they show how marginality and -extremization constrain R-charges to reproduce gravity results, providing strong evidence for the AdS/CFT dictionary in these settings. The work also highlights the tractability of non-chiral models and discusses limitations and future directions for chiral theories.

Abstract

We test the AdS/CFT correspondence by computing the partition function of some quiver Chern-Simons-matter theories on three-sphere. The M-theory backgrounds are of the Freund-Rubin type with the seven-dimensional internal space given as Sasaki-Einstein manifolds or . Localization technique reduces the exact path integral to a matrix model, and we study the large-N behavior of the partition function. For simplicity we consider only non-chiral models which have a real-valued partition function. The result is in full agreement with the prediction of the gravity duals, i.e. the free energy is proportional to and the coefficient matches correctly the volume of and .

Paper Structure

This paper contains 6 sections, 52 equations, 9 figures.

Figures (9)

  • Figure 1: The quiver diagram for Chern-Simons dual of $AdS_4 \times V^{5,2}$
  • Figure 2:
  • Figure 3: These figures show the density of roots $\rho(x)$ for $V^{5,2}$. The dots are numerical data and the red lines show the analytical predictions.
  • Figure 4: The quiver diagram for Chern-Simons dual of $AdS_4 \times Q^{1,1,1}$
  • Figure 5: The distribution of roots for $Q^{1,1,1}$ theory with different R charges. The roots are plotted with black and blue dots for $N=20$ and $100$, respectively. The real part of the roots scales as $\sqrt{N}$. The maximum values of imaginary part of $\lambda$ are bounded by $\pi\Delta_B$, which are represented by green lines.
  • ...and 4 more figures