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Intersecting D-branes and Lifshitz-like space-time

High Energy Physics - Theory · Submitted 22 Apr 2012

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

The authors' main claim In this paper we show that similar structures also arise from the near horizon limit of 1/4 BPS, threshold intersecting D-brane solutions of type II string theories.

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arXiv ID1204.4858 (version 2)
Pith IDFIQK27Y5, Pith's permanent record of this paper and its review
CitationParijat Dey, Shibaji Roy. "Intersecting D-branes and Lifshitz-like space-time." arXiv:1204.4858 (2012). https://pith.science/paper/FIQK27Y5
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What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.88 · human participants 0.01 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.09 · compares with prior results 0.94 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

In a previous paper (Dey and Roy, arXiv:1203.5381) we have shown how Lifshitz-like space-times (space-times having Lifshitz scaling with hyperscaling violation) arise from 1/4 BPS, threshold F-D$p$ bound state solutions of type II string theories in the near horizon limit. In this paper we show that similar structures also arise from the near horizon limit of 1/4 BPS, threshold intersecting D-brane solutions of type II string theories. Some of these solutions are standard (D$p$-D($p+4$) for $p=0, 2$) and some are non-standard (D$p$-D($p+2)$ for $p = 1, 2, 3$) including D2-D2$'$, D3-D3$'$ and D4-D4$'$ solutions. The dilatons of these solutions in general run (except in D2-D4 and D3-D3$'$ cases) and produce RG flows. We discuss the phase structures of these solutions. D2-D4 and D3-D3$'$ in the near horizon limit do not produce Lifshitz-like space-time, but give AdS$_3$ spaces.

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 a previous paper (Dey and Roy, arXiv:1203.5381) we have shown how Lifshitz-like space-times (space-times having Lifshitz scaling with hyperscaling violation) arise from 1/4 BPS, threshold F-D$p$ bound state solutions of type II string theories in the near horizon limit. background 1.00 0.42 0.04 asserted 1.00
s1 In this paper we show that similar structures also arise from the near horizon limit of 1/4 BPS, threshold intersecting D-brane solutions of type II string theories. contribution 0.90 0.94 0.86 asserted 1.00
s2 Some of these solutions are standard (D$p$-D($p+4$) for $p=0, 2$) and some are non-standard (D$p$-D($p+2)$ for $p = 1, 2, 3$) including D2-D2$'$, D3-D3$'$ and D4-D4$'$ solutions. contribution 0.85 0.75 0.10 asserted 1.00
s3 The dilatons of these solutions in general run (except in D2-D4 and D3-D3$'$ cases) and produce RG flows. result 0.93 0.84 0.05 asserted 1.00
s4 We discuss the phase structures of these solutions. contribution 0.99 0.86 0.04 asserted 0.56
s5 D2-D4 and D3-D3$'$ in the near horizon limit do not produce Lifshitz-like space-time, but give AdS$_3$ spaces. result 0.96 0.88 0.11 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.99.

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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 a previous paper (Dey and Roy, arXiv:1203.5381) we have shown how Lifshitz-like space-times (space-times having Lifshitz scaling with hyperscaling violation) arise from 1/4 BPS, threshold F-D$p$ bound state solutions of type II string theories in the near horizon limit. In this paper we show that similar structures also arise from the near horizon limit of 1/4 BPS, threshold intersecting D-brane solutions of type II string theories. Some of these solutions are standard (D$p$-D($p+4$) for $p=0, 2$) and some are non-standard (D$p$-D($p+2)$ for $p = 1, 2, 3$) including D2-D2$'$, D3-D3$'$ and D4-D4$'$ solutions. The dilatons of these solutions in general run (except in D2-D4 and D3-D3$'$ cases) and produce RG flows. We discuss the phase structures of these solutions. D2-D4 and D3-D3$'$ in the near horizon limit do not produce Lifshitz-like space-time, but give AdS$_3$ spaces.

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References
How the literature uses it

21 arXiv papers cite this in 31 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 · 21 sentences without a confident label

Compares with it 1 paper
Cites it as background 9 papers
  • Among them the ones which yield AdS$_3$ (AdS$_2$ is excluded as we mentioned) geometry are M2 $⊥$ M5 and M5 $⊥$ M5 $⊥$ M5 [ref] of M-theory and D1 $⊥$ D5, D2 $⊥$ D4, D3 $⊥$ D3 and F $⊥$ NS5 [ref] of type II string theories (the solutions involving triple intersections of string theory branes are not known explicitly and even if they give AdS geometry, they will either give AdS$_3$ or AdS$_2$ similar to the solutions involving double intersections and therefore we will not consider them here to avoid repetitions).

    From AdS to Schr\"odinger/Lifshitz dual space-times without or with hyperscaling violation · Introduction · 0.81

  • By now there exist various holographic dual models for critical points involving Lifschitz scaling and hyperscaling violation [ref] .

    Holographic thermalization with Lifshitz scaling and hyperscaling violation · Introduction · 0.97

  • For example, see [ref] for discussions on how black hole no-hair theorems can be violated in AdS space in the context of holographic superconductivity; [ref] for discussions of how emergent horizons with properties reflecting dynamical scaling in the dual field theory (“Lifshitz solutions") can arise; and [ref] for discussions of horizons exhibiting both dynamical scaling and hyperscaling violation.[Embeddings of such solutions in string theory have also been discussed in many papers, such as [ref] .] The earliest work mostly focused on horizons with translational and rotational symmetry, but more recently examples of black brane horizons dual to field theories with further reduced space-time symmetries have been discussed in e.g. [ref] .

    Interpolating from Bianchi Attractors to Lifshitz and AdS Spacetimes · Introduction · 0.89

What it cites · 26 sentences without a confident label

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