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From Schurs to Giants in ABJ(M)
High Energy Physics - Theory · Submitted 29 Oct 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our analysis imposes several constraints on the physics of the probe branes on AdS4xCP3 as well as sheds more light on giant graviton solutions in this background with additional NS B-field.
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The abstract, sentence by sentence
In this work we consider various correlators with Schur polynomials in ABJ(M) models that on the dual gravity side should correspond to processes involving giant gravitons. Our analysis imposes several constraints on the physics of the probe branes on AdS4xCP3 as well as sheds more light on giant graviton solutions in this background with additional NS B-field. Our main tool is a formula that we derive for extremal n-point functions of the single trace chiral primary operators in the free field theory limit. The formula expresses the correlators in terms of the two-point function of Schur polynomials labeled by hook diagrams and is valid for a large class of gauge theories. In particular, in N = 4 SYM, it proves the conjecture of Beisert et al.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this work we consider various correlators with Schur polynomials in ABJ(M) models that on the dual gravity side should correspond to processes involving giant gravitons. | contribution 0.92 | 0.70 | 0.10 | hedged possibility 0.60 |
| s1 | Our analysis imposes several constraints on the physics of the probe branes on AdS4xCP3 as well as sheds more light on giant graviton solutions in this background with additional NS B-field. | interpretation 0.56 | 0.87 | 0.19 | asserted 0.98 |
| s2 | Our main tool is a formula that we derive for extremal n-point functions of the single trace chiral primary operators in the free field theory limit. | method 0.94 | 0.96 | 0.12 | asserted 1.00 |
| s3 | The formula expresses the correlators in terms of the two-point function of Schur polynomials labeled by hook diagrams and is valid for a large class of gauge theories. | result 0.41 | 0.92 | 0.18 | asserted 1.00 |
| s4 | In particular, in N = 4 SYM, it proves the conjecture of Beisert et al. | result 0.94 | 0.76 | 0.19 | asserted 1.00 |
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The paper
Original abstract
In this work we consider various correlators with Schur polynomials in ABJ(M) models that on the dual gravity side should correspond to processes involving giant gravitons. Our analysis imposes several constraints on the physics of the probe branes on AdS4xCP3 as well as sheds more light on giant graviton solutions in this background with additional NS B-field. Our main tool is a formula that we derive for extremal n-point functions of the single trace chiral primary operators in the free field theory limit. The formula expresses the correlators in terms of the two-point function of Schur polynomials labeled by hook diagrams and is valid for a large class of gauge theories. In particular, in N = 4 SYM, it proves the conjecture of Beisert et al.
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References
How the literature uses it
13 arXiv papers cite this in 17 sentences
Papers citing it · 11 sentences without a confident label
Builds on it 3 papers
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This again generalizes results that are known for the $U(N)$ gauge theory [ref] .
A basis for large operators in N=4 SYM with orthogonal gauge group · Introduction · 0.96
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This provides a complete generalization of the $U(N)$ result which was derived in [ref] .
Operators, Correlators and Free Fermions for SO(N) and Sp(N) · Multi trace Correlators Again · 0.95
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This procedure can be generalized easily to the case when the gauge groups have different rank [ref] , by multiplying the results of these products of numbers when we decorate the Young diagrams with the ranks for each gauge group in the chain instead of a common one $N$.
Extremal chiral ring states in AdS/CFT are described by free fermions for a generalized oscillator algebra · Extremal chiral ring states are described by Young diagrams · 0.86
Cites it as background 3 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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For the theory with gauge group $U(N)$ the technology for computing n-point correlators is rather well developed [ref] .
A basis for large operators in N=4 SYM with orthogonal gauge group · Discussion and future directions · 0.93
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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 · 31 sentences without a confident label
Builds on 1 paper
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After detailed analysis we put forward a prediction for the ABJ giant graviton solution that remains to be constructed and should generalize [ref] .
The giant graviton on AdS_{4} x CP^{3} - another step towards the emergence of geometry · Introduction and summary · 0.98
Uses the method or tool of 1 paper
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The amplitude can be computed using appendix H of [ref] for ABJ operators together with the results obtained in our appendix D, we consider the case where both $R$ and $S$ have rows of $O(N)$ and columns of $O(1)$ (the other case follows directly by changing to the symmetric representation).
Giant Gravitons - with Strings Attached (III) · String splitting and joining · 0.91
Compares with 3 papers
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Mathematica can formally sum it into a combination of the Meijer G-functions [equation] To the leading order in $N$ and $M$ and the answer is [equation] Using this result we can compute the normalized three point functions [equation] This leading contribution was also computed in [ref] and it is equal to the sum of two leading $𝒩=4$ three point functions in $N$ and $M$.
Correlators of Giant Gravitons from dual ABJ(M) Theory · Three-point functions · 0.99
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That is [equation] Upon using equation [ref], we get [equation] Shifting $J_1$ to $J_1+1$, we arrive at [equation] Similarly [equation] Recall the result of open string correlators in $N=4$ SYM theory [ref] [equation] once again, ABJ answer is not simply a product of two open string correlators.
Giant Gravitons - with Strings Attached (III) · Open string correlators · 0.92
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If we set $N=M$ our coefficients reduce to the extremal three correlators in ABJM that were studied in [ref] both in gauge theory and gravity.
Giant Gravitons on AdS_4 x CP^3 and their Holographic Three-point Functions · Two Schurs and a CPO · 0.97
Cites as background 17 papers
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One of the most important developments in this direction is the new $AdS_4/CFT_3$ duality proposed by Aharony, Jafferis, Bergman and Maldacena (ABJM) [ref] .
N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals · Brief review of the ABJ(M) models · 0.97
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Three-dimensional ABJ(M) models [ref] are conjectured to capture the physics of M-branes in $AdS_4×S^7$ and D-branes in type IIA theory on $AdS_4×ℂℙ^3$.
Fractional M2-branes · Introduction and summary · 0.83
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For more details see [ref] .
ABJM Baryon Stability and Myers effect · Schurs and giants in $AdS_4/CFT_3$ · 0.96
Discussion
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