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Yang-Mills- and D-instantons

High Energy Physics - Theory · Submitted 26 Apr 2000

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim By taking the D-instantons to live in an $AdS_5\times S^5$ background, we perform explicit checks of the AdS/CFT correspondence.

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arXiv IDhep-th/0004186 (version 2)
Pith ID7LF2I4KJ, Pith's permanent record of this paper and its review
CitationA.V. Belitsky, P. van Nieuwenhuizen, S. Vandoren. "Yang-Mills- and D-instantons." arXiv:hep-th/0004186 (2000). https://pith.science/paper/7LF2I4KJ
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,630 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.22 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.16 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

In these lectures, which are written at an elementary and pedagogical level, we discuss general aspects of (single) instantons in SU(N_c) Yang-Mills theory, and then specialize to the case of N = 4 supersymmetry and the large N_c limit. We show how to determine the measure of collective coordinates and compute instanton corrections to certain correlation functions. We then relate this to D-instantons in type IIB supergravity. By taking the D-instantons to live in an $AdS_5\times S^5$ background, we perform explicit checks of the AdS/CFT correspondence.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 In these lectures, which are written at an elementary and pedagogical level, we discuss general aspects of (single) instantons in SU(N_c) Yang-Mills theory, and then specialize to the case of N = 4 supersymmetry and the large N_c limit. contribution 0.68 0.48 0.05 asserted 0.87
s1 We show how to determine the measure of collective coordinates and compute instanton corrections to certain correlation functions. contribution 0.50 0.92 0.08 asserted 1.00
s2 We then relate this to D-instantons in type IIB supergravity. contribution 0.88 0.77 0.09 asserted 0.98
s3 By taking the D-instantons to live in an $AdS_5\times S^5$ background, we perform explicit checks of the AdS/CFT correspondence. contribution 0.44 0.90 0.33 asserted 1.00

What kind of paper the classifier reports this is: review 0.65 · evidence from proof or derivation 0.98.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In these lectures, which are written at an elementary and pedagogical level, we discuss general aspects of (single) instantons in SU(N_c) Yang-Mills theory, and then specialize to the case of N = 4 supersymmetry and the large N_c limit. We show how to determine the measure of collective coordinates and compute instanton corrections to certain correlation functions. We then relate this to D-instantons in type IIB supergravity. By taking the D-instantons to live in an $AdS_5\times S^5$ background, we perform explicit checks of the AdS/CFT correspondence.

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References
How the literature uses it

15 arXiv papers cite this in 25 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 15 sentences without a confident label

Uses its method or tool 2 papers
  • In principle, starting from our bosonic solution, we can construct a solution with fermions turned on by performing a finite supersymmetry transformation - sometimes referred to as the sweeping procedure [ref] .

    Supersymmetric Soliton $\sigma$-models from Non-Lorentzian Field Theories · Solving the constraints · 0.97

  • A convenient representation for $d=6$ gamma matrices can be built starting with 't Hooft symbols (see appendices in [ref] ) η_a m n = _a m n 4+_a m_n 4-_a n_m 4 η_a m n = _a m n 4-_a m_n 4+_a n_m 4 , where $a=1,2,3$ (only in this and the next appendix) and $m=1,2,3,4$.

    Dynamical supersymmetry in maximally supersymmetric gauge theories · 't Hooft symbols and $d=6$ gamma matrices · 0.86

Uses its data or values 1 paper
Cites it as background 5 papers
  • N=4 SYM at strong coupling is related via the AdS/CFT correspondence [ref] to the supergravity in ten dimensions with the following action (in Euclidean formulation) [ref] [The action of SG1 is written for ten dimrensional flat space ($R10$).

    D-instantons and multiparticle production in N=4 SYM · Supergravity (boson sector) · 0.90

  • Historically the string theoretic derivation [ref] of the famous ADHM construction of gauge instantons [ref] was among the first appearances of Euclidean D-branes in the context of instanton computations and has been the subject of many early investigations including [ref] (for reviews and more references see [ref] ).

    D-brane Instantons in Type II String Theory · ADS superpotential for $SU(N_c)$ SQCD · 0.99

  • The solution constructed iteratively in this way is called super-instanton (cf. [ref] for reviews).

    Generalized instantons in N = 4 super Yang-Mills theory and spinorial geometry · Euclidean $N=4$ SYM theory and instantons · 0.98

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