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Instanton Effects in ABJM Theory from Fermi Gas Approach (1211.1251v2)

Published 6 Nov 2012 in hep-th

Abstract: We study the instanton effects of the ABJM partition function using the Fermi gas formalism. We compute the exact values of the partition function at the Chern-Simons levels k=1,2,3,4,6 up to N=44,20,18,16,14 respectively, and extract non-perturbative corrections from these exact results. Fitting the resulting non-perturbative corrections by their expected forms from the Fermi gas, we determine unknown parameters in them. After separating the oscillating behavior of the grand potential, which originates in the periodicity of the grand partition function, and the worldsheet instanton contribution, which is computed from the topological string theory, we succeed in proposing an analytical expression for the leading D2-instanton correction. Just as the perturbative result, the instanton corrections to the partition function are expressed in terms of the Airy function.

Citations (212)

Summary

  • The paper demonstrates that instanton contributions to the ABJM partition function closely align with the Airy function predictions.
  • Using the Fermi gas formalism, the authors extract precise D2-instanton corrections by isolating oscillatory behavior from the grand potential.
  • The research provides an analytical toolkit for understanding non-perturbative effects, offering insights into large N dynamics and gauge-gravity duality.

Overview of "Instanton Effects in ABJM Theory from Fermi Gas Approach"

The paper entitled "Instanton Effects in ABJM Theory from Fermi Gas Approach" is an in-depth paper of non-perturbative contributions to the partition function of the ABJM model, employing the Fermi gas formalism. The authors Hatsuda, Moriyama, and Okuyama have computed the exact values of the partition function at various Chern-Simons levels, specifically k=1,2,3,4,6k = 1, 2, 3, 4, 6, and for large matrix sizes up to N=44,20,18,16,14N=44, 20, 18, 16, 14, respectively. These computations allow for extracting non-perturbative corrections through the Fermi gas methodology.

This research builds on the transition of ABJM theory into a Fermi gas system, illustrating how instanton effects can be teased out from the exact partition function. The methodology hinges upon converting the problem into a grand potential framework, followed by the separation and analysis of oscillatory behavior from worldsheet instanton corrections.

Key Numerical Findings

From the exact results for the partition function, the research highlights several significant numerical findings:

  • For k=1,2,3,4,6k=1,2,3,4,6, the perturbative and leading instanton corrections to the partition function fit precisely with the expected pattern based on the Airy function's form. This finding demonstrates the power of using a Fermi gas approach to describe non-perturbative effects comprehensively.
  • The leading corrections (D2-instanton) are revealed through careful oscillation removal from the grand potential and subsequent numerical fitting. This yields precise values for unknown parameters characterizing the non-perturbative contributions.

Implications and Theoretical Contributions

This research offers significant insights into M-theory, particularly how partition functions can capture both perturbative and instanton effects in a coherent analytical structure using the Fermi gas formalism. The results bear implications for understanding large NN limit behaviors and the dual properties in topological string theory and gauge-gravity duality.

The paper proposes analytic forms for D2-instanton contributions, showing consistency across multiple Chern-Simons levels and providing an enhanced understanding compared to previous speculative approaches. This conjecture holds potential for further guiding theoretical explorations in quantum field theories and string theory.

Speculation on Future Developments

The methods and results from this paper lay the groundwork for more expansive generalizations to other multi-instanton sectors. Future exploration may focus on determining how higher-order instanton contributions relate to bound states, potentially extending to broader classes of gauge theories and higher-dimensional matrix models.

Moreover, the interplay between the oscillatory nature of the grand potential and non-perturbative sums suggests potential new directions in topological string theory, offering a richer tapestry of mathematical structures to explore. Progress in these areas could potentially illuminate deeper symmetries and invariants in M-theory and string theory frameworks.

In summary, this paper delivers a valuable analytical toolkit to accurately quantify non-perturbative effects using the Fermi gas perspective, offering new mathematical structures to the symphony of M-theory and quantum gravity research.