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D-branes as Solitons of an N=1, D=10 Non-commutative Gauge Theory

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M. Mihailescu, I.Y. Park, T.A. Tran

High Energy Physics - Theory · Submitted 9 Nov 2000

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

The authors' main claim These results indicate that the soliton solution is the low energy realization of a D3 brane in a D9 brane with a transverse B-field, hence can be viewed as a generalization of the previous results in the literature where similar observations were made for lower codimensional cases.

how it is stated · hedged possibility 0.99 read the record →

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arXiv IDhep-th/0011079 (version 3)
Pith IDU4PKK4Y5, Pith's permanent record of this paper and its review
CitationI.Y. Park, M. Mihailescu, T.A. Tran. "D-branes as Solitons of an N=1, D=10 Non-commutative Gauge Theory." arXiv:hep-th/0011079 (2000). https://pith.science/paper/U4PKK4Y5
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The compiled record

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, 3,732 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.14 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.91 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v3. Results and the main claim are underlined; .

We consider a Dp brane within a D9 brane in the presence of a B-field whose polarization is {\em transverse} to the Dp brane. To be definite, we take a D3-D9 system. It is observed that the system has the same pattern of supersymmetry breaking as that of a soliton of the six dimensional non-commutative gauge theory that is obtained by dimensional reduction of an {\cal N}=1, D=10 gauge theory. These results indicate that the soliton solution is the low energy realization of a D3 brane in a D9 brane with a transverse B-field, hence can be viewed as a generalization of the previous results in the literature where similar observations were made for lower codimensional cases.

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 consider a Dp brane within a D9 brane in the presence of a B-field whose polarization is {\em transverse} to the Dp brane. contribution 0.56 0.28 0.04 asserted 0.83
s1 To be definite, we take a D3-D9 system. method 0.58 0.61 0.03 asserted 0.89
s2 It is observed that the system has the same pattern of supersymmetry breaking as that of a soliton of the six dimensional non-commutative gauge theory that is obtained by dimensional reduction of an {\cal N}=1, D=10 gauge theory. result 0.99 0.46 0.25 asserted 0.97
s3 These results indicate that the soliton solution is the low energy realization of a D3 brane in a D9 brane with a transverse B-field, hence can be viewed as a generalization of the previous results in the literature where similar observations were made for lower codimensional cases. interpretation 1.00 0.71 0.84 hedged possibility 0.99

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.52.

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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 consider a Dp brane within a D9 brane in the presence of a B-field whose polarization is {\em transverse} to the Dp brane. To be definite, we take a D3-D9 system. It is observed that the system has the same pattern of supersymmetry breaking as that of a soliton of the six dimensional non-commutative gauge theory that is obtained by dimensional reduction of an {\cal N}=1, D=10 gauge theory. These results indicate that the soliton solution is the low energy realization of a D3 brane in a D9 brane with a transverse B-field, hence can be viewed as a generalization of the previous results in the literature where similar observations were made for lower codimensional cases.

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References
How the literature uses it

12 arXiv papers cite this in 13 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 · 8 sentences without a confident label

Uses its method or tool 1 paper
  • In general, this choice of flux will break supersymmetry on the D8-brane, though the D0-brane may still experience an effective supersymmetric quantum mechanics.[Following [ref] , to study the unbroken supersymmetries in the presence of this flux, introduce the block diagonal matrix $M$ in the $8_v$ representation (see e.g. [ref] ): M=i=14⊕M_i, M_i=[ [ cos2πv_i sin2πv_i; -sin2πv_i cos2πv_i ] ] . where each $v_j$ is given by: exp2πiv_j=1+if_j/1-if_j.

    Instantons, Twistors, and Emergent Gravity · Brane Construction · 0.88

Cites it as background 4 papers
  • Other than the well known Freund-Rubin $AdS_4×S^6$ vacua [ref] , some supersymmetric solutions of the theory include D8-branes [ref] , the $K3$ compactifications [ref] , the $(D6,D8)$ and $(D4,D6,D8)$ bound states [ref] .

    RG flows and cascades of $Lif_4^{(2)}\times S^1\times S^5$ vacua · $Lif^(2)_4×S^1×S^5$ vacua · 0.92

  • The problem of adhering $D0$-branes to $D6$-branes in a supersymmetric manner was first considered by Witten [ref] [See also related work in [ref] .].

    Constituent Model of Extremal non-BPS Black Holes · Multi-center BPS solutions and decay of the non-BPS $D0-D6$ black holes · 0.97

  • Other than the nonsupersymmetric Freund-Rubin vacua in [ref] , some known BPS solutions of the theory include D8-branes [ref] , the $K3$ compactifications [ref] , the $(D6,D8)$ and $(D4,D6,D8)$ bound states [ref] .

    D2-D8 system with massive strings and the Lifshitz spacetimes · $Sch_4^(3)×S^6$: massive strings · 0.94

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