2013
DOI: 10.1007/jhep05(2013)054
|View full text |Cite
|
Sign up to set email alerts
|

Instanton bound states in ABJM theory

Abstract: The partition function of the ABJM theory receives non-perturbative corrections due to instanton effects. We study these non-perturbative corrections, including bound states of worldsheet instantons and membrane instantons, in the Fermi-gas approach. We require that the total non-perturbative correction should be always finite for arbitrary Chern-Simons level. This finiteness is realized quite non-trivially because each bound state contribution naively diverges at some levels. The poles of each contribution sh… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

6
208
0

Year Published

2015
2015
2023
2023

Publication Types

Select...
8
1

Relationship

5
4

Authors

Journals

citations
Cited by 117 publications
(222 citation statements)
references
References 44 publications
(123 reference statements)
6
208
0
Order By: Relevance
“…(µ), the perturbative part is given by 16) with the coefficients 17) and the bound states are completely taken care of by the worldsheet instantons and the nonperturbative part consists only of pure worldsheet instantons and pure membrane instantons …”
Section: Jhep08(2017)003mentioning
confidence: 99%
See 1 more Smart Citation
“…(µ), the perturbative part is given by 16) with the coefficients 17) and the bound states are completely taken care of by the worldsheet instantons and the nonperturbative part consists only of pure worldsheet instantons and pure membrane instantons …”
Section: Jhep08(2017)003mentioning
confidence: 99%
“…After the discovery of the Fermi gas formalism [11] which rewrites the partition function into that of a Fermi gas system with N particles, more information on the matrix model was obtained. Besides the 't Hooft expansion, we can perform the WKB small k expansion [11,12] or study the numerical fitting from the exact values of the partition function [13][14][15][16]. Finally, the non-perturbative effects of the matrix model in the grand canonical ensemble are given explicitly by the free energy of the topological string theory on the local P 1 × P 1 geometry [8,9,17].…”
Section: Introductionmentioning
confidence: 99%
“…Inspired by the seminal work of Drukker, Marino, and Putrov [71,72] and, in good part, with the use of the elegant Fermi gas approach developed by Marino and Putrov [73], a great deal about the ABJ(M) partition function has been uncovered, in particular, at large N , both in perturbative [73,74] and nonperturbative expansions [75][76][77][78][79][80][81][82]. There has also been significant progress in the study of Wilson loops in the ABJ(M) theory [83][84][85][86] as well as the partition functions of more general Chern-Simons-matter theories [87][88][89][90][91].…”
Section: Jhep08(2016)174mentioning
confidence: 99%
“…From a series of works [13,14,15,16,11,17,18,19,20,21,22], we have found the grand potential of the ABJM partition function defined by…”
Section: Exact Instanton Expansionsmentioning
confidence: 99%