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Nonplanar Integrability and Parity in ABJ Theory
High Energy Physics - Theory · Submitted 30 Jul 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our analysis shows that (M-N) is related to the holonomy in the string theory, confirming one of the main features of the theory and its string dual.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
In this article we study the action of the non-planar two-loop dilatation operator in an SU(2)*SU(2) sub-sector of the ABJ Chern-Simons-matter theory. The gauge invariant operators we consider are the restricted Schur polynomials. As in ABJM theory, there is a limit in which the spectrum reduces to a set of decoupled harmonic oscillators, indicating integrability in the large M and N double limit of the theory. We then consider parity transformations on the gauge invariant operators. In this case the non-planar anomalous dimensions break parity invariance. Our analysis shows that (M-N) is related to the holonomy in the string theory, confirming one of the main features of the theory and its string dual. Furthermore, in the limit where ABJ theory reduces to ABJM theory, parity invariance is restored.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this article we study the action of the non-planar two-loop dilatation operator in an SU(2)*SU(2) sub-sector of the ABJ Chern-Simons-matter theory. | contribution 0.99 | 0.87 | 0.04 | asserted 0.74 |
| s1 | The gauge invariant operators we consider are the restricted Schur polynomials. | method 0.54 | 0.36 | 0.02 | asserted 1.00 |
| s2 | As in ABJM theory, there is a limit in which the spectrum reduces to a set of decoupled harmonic oscillators, indicating integrability in the large M and N double limit of the theory. | result 0.92 | 0.56 | 0.19 | hedged possibility 0.71 |
| s3 | We then consider parity transformations on the gauge invariant operators. | contribution 0.96 | 0.81 | 0.03 | asserted 0.63 |
| s4 | In this case the non-planar anomalous dimensions break parity invariance. | result 1.00 | 0.81 | 0.24 | asserted 1.00 |
| s5 | Our analysis shows that (M-N) is related to the holonomy in the string theory, confirming one of the main features of the theory and its string dual. | result 0.62 | 0.85 | 0.40 | asserted 1.00 |
| s6 | Furthermore, in the limit where ABJ theory reduces to ABJM theory, parity invariance is restored. | result 0.98 | 0.78 | 0.15 | asserted 1.00 |
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The paper
Original abstract
In this article we study the action of the non-planar two-loop dilatation operator in an SU(2)*SU(2) sub-sector of the ABJ Chern-Simons-matter theory. The gauge invariant operators we consider are the restricted Schur polynomials. As in ABJM theory, there is a limit in which the spectrum reduces to a set of decoupled harmonic oscillators, indicating integrability in the large M and N double limit of the theory. We then consider parity transformations on the gauge invariant operators. In this case the non-planar anomalous dimensions break parity invariance. Our analysis shows that (M-N) is related to the holonomy in the string theory, confirming one of the main features of the theory and its string dual. Furthermore, in the limit where ABJ theory reduces to ABJM theory, parity invariance is restored.
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How the literature uses it
5 arXiv papers cite this in 5 sentences
Papers citing it · 3 sentences without a confident label
Cites it as background 2 papers
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For quiver gauge theories, there are two distinct approaches that have been developed to study the finite $N$ physics [ref] [For earlier work, focusing on essentially single matrix dynamics, see [ref] ].
Finite N Quiver Gauge Theory · Summary and Conclusions · 0.97
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The studies were extended beyond $=4$ SYM to gauge theories such as ABJM [ref] and the conifold [ref] .
Quivers, Words and Fundamentals · Introduction · 0.80
What it cites · 35 sentences without a confident label
Compares with 6 papers
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The computation of [ref] gives [equation] [equation] [equation] [equation] where [equation] The combination $Ô_j,j^3(b_0,b_1)$ in [ref] differs from the ones obtained in the case of $N=4$ SYM theory and ABJM theory [ref] , since it depends on both $M$ and $N$.
Beyond the Planar Limit in ABJM · Spectrum of Anomalous Dimensions · 0.91
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The computation of [ref] gives [equation] [equation] [equation] [equation] where [equation] The combination $Ô_j,j^3(b_0,b_1)$ in [ref] differs from the ones obtained in the case of $N=4$ SYM theory and ABJM theory [ref] , since it depends on both $M$ and $N$.
Nonplanar Integrability · Spectrum of Anomalous Dimensions · 0.91
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In contrast to this, the spin chains technique for ABJM which is relevant for expansion about the planar limit of the theory did not find any sign of non-planar integrability [ref] .
Non-planar ABJM Theory and Integrability · Introduction · 0.88
Cites as background 1 paper
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The first example involves ABJM theory with gauge group $U(N)_k×U(N)_-k$, where $k$ denotes the Chern-Simons level [ref] .
N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals · Introduction · 0.97
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