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1/8 BPS States in Ads/CFT

High Energy Physics - Theory · Submitted 6 Nov 2006

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

The authors' main claim We analyze the solutions to these equations in a large radius asymptotic expansion: they carry charges with respect to two U(1) KK gauge fields and their mass saturates the expected BPS bound.

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arXiv IDhep-th/0611065 (version 2)
Pith IDQOBEVILC, Pith's permanent record of this paper and its review
CitationE. Gava, G. Milanesi, K.S. Narain, M. O'Loughlin. "1/8 BPS States in Ads/CFT." arXiv:hep-th/0611065 (2006). https://pith.science/paper/QOBEVILC
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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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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,303 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.16 · human participants 0.01 · controlled comparison 0.01 · randomized assignment 0.01 · states quantitative result 0.85 · compares with prior results 0.07 · mentions code or data availability 0.01.

The abstract, sentence by sentence

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

We study a class of exact supersymmetric solutions of type IIB Supergravity. They have an SO(4) x SU(2) x U(1) isometry and preserve generically 4 of the 32 supersymmetries of the theory. Asymptotically AdS_5 x S^5 solutions in this class are dual to 1/8 BPS chiral operators which preserve the same symmetries in the N=4 SYM theory. They are parametrized by a set of four functions that satisfy certain differential equations. We analyze the solutions to these equations in a large radius asymptotic expansion: they carry charges with respect to two U(1) KK gauge fields and their mass saturates the expected BPS bound.

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 We study a class of exact supersymmetric solutions of type IIB Supergravity. contribution 0.99 0.91 0.05 asserted 0.99
s1 They have an SO(4) x SU(2) x U(1) isometry and preserve generically 4 of the 32 supersymmetries of the theory. result 0.76 0.53 0.08 asserted 0.96
s2 Asymptotically AdS_5 x S^5 solutions in this class are dual to 1/8 BPS chiral operators which preserve the same symmetries in the N=4 SYM theory. interpretation 0.81 0.38 0.34 asserted 1.00
s3 They are parametrized by a set of four functions that satisfy certain differential equations. contribution 0.43 0.45 0.07 asserted 1.00
s4 We analyze the solutions to these equations in a large radius asymptotic expansion: they carry charges with respect to two U(1) KK gauge fields and their mass saturates the expected BPS bound. result 0.89 0.91 0.36 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

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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

We study a class of exact supersymmetric solutions of type IIB Supergravity. They have an SO(4) x SU(2) x U(1) isometry and preserve generically 4 of the 32 supersymmetries of the theory. Asymptotically AdS_5 x S^5 solutions in this class are dual to 1/8 BPS chiral operators which preserve the same symmetries in the N=4 SYM theory. They are parametrized by a set of four functions that satisfy certain differential equations. We analyze the solutions to these equations in a large radius asymptotic expansion: they carry charges with respect to two U(1) KK gauge fields and their mass saturates the expected BPS bound.

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References
How the literature uses it

18 arXiv papers cite this in 43 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 · 23 sentences without a confident label

Contests it 1 paper
  • The purpose of this section is to examine the result of [ref] and point out the existence of an additional constraint [ref].

    Liouville Equation in 1/8 BPS Geometries · 1/8 BPS geometries with $SU(2)×U(1)×SO(4)×R$ · contest 0.71

Builds on it 2 papers
  • In this paper we first show in detail how to recover the $AdS_5×Y^p,q$ geometries from the generic solutions studied in [ref] by requiring that additional 4 supercharges be preserved.

    Half BPS states in AdS_5 x Y^{p,q} · Introduction · 0.96

  • In this paper, we have shown that a new differential equation should be imposed on the resultant controlling functions $m,n,p,T$ of [ref] , and discussed the limit $n=0,m=1/y^2$, in which the new equation plays crucial roles to obtain some properties of the geometries.

    Liouville Equation in 1/8 BPS Geometries · Conclusion · 0.84

Cites it as background 10 papers
  • Among them we concentrate on the result of [ref] , in which the case of $SU(2)×U(1)×SO(4)×R$ symmetry was studied and as a result, a class of $1/8$ BPS geometries were written in terms of four functions and four differential equations for them have been found.

    Liouville Equation in 1/8 BPS Geometries · Introduction · 0.80

  • In Section [ref] we give a brief summary of the results of [ref] .

    Half BPS states in AdS_5 x Y^{p,q} · Introduction · 0.95

  • The geometries corresponding to such BPS states have been studied in [ref] and in [ref] , [ref] , [ref] (see also related discussion [ref] , [ref] ), which is a $R_t [equation] z_3/z_1 →z_3$), [equation] Near the circle $|z_1|≈1,$ we see that $|z_2|^2+|z_3|^2 ≈ϵ^2,$so the $S^3$in$z_2,z_3$ space shrinks at the boundary of $D^2$ in $z_1$ space.

    Studies on 1/4 BPS and 1/8 BPS geometries · Small variation · 0.85

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