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M-theory compactified on Calabi-Yau fourfolds with background flux

High Energy Physics - Theory · Submitted 9 Mar 2001

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The authors' main claim The resulting scalar- and superpotential is computed and compared with the superpotential obtained by Gukov, Vafa and Witten using different methods.

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arXiv IDhep-th/0103068 (version 2)
Pith IDKRAKK3WZ, Pith's permanent record of this paper and its review
CitationJan Louis, Michael Haack. "M-theory compactified on Calabi-Yau fourfolds with background flux." arXiv:hep-th/0103068 (2001). https://pith.science/paper/KRAKK3WZ
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.06 · human participants 0.01 · controlled comparison 0.12 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.98 · mentions code or data availability 0.01.

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

We perform the Kaluza-Klein reduction of M-theory on warped Calabi-Yau fourfolds with non-trivial four-form flux turned on. The resulting scalar- and superpotential is computed and compared with the superpotential obtained by Gukov, Vafa and Witten using different methods.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We perform the Kaluza-Klein reduction of M-theory on warped Calabi-Yau fourfolds with non-trivial four-form flux turned on. method 0.60 0.95 0.07 asserted 1.00
s1 The resulting scalar- and superpotential is computed and compared with the superpotential obtained by Gukov, Vafa and Witten using different methods. result 0.76 0.86 0.32 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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The paper
Original abstract

We perform the Kaluza-Klein reduction of M-theory on warped Calabi-Yau fourfolds with non-trivial four-form flux turned on. The resulting scalar- and superpotential is computed and compared with the superpotential obtained by Gukov, Vafa and Witten using different methods.

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References
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45 arXiv papers cite this in 93 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 · 64 sentences without a confident label

Uses its method or tool 3 papers
  • Using [ref], one performs the dimensional reduction of the classical part of [ref], see [ref] , and finds [equation] To rewrite expressions in terms of the quantities introduced in [ref] and [ref], one makes use of identities valid for the Hodge star $*_8$ evaluated on certain internal harmonic forms.

    From M-theory higher curvature terms to \alpha' corrections in F-theory · Dimensional reduction of higher-curvature terms · 0.97

  • We begin our analysis in Section [ref] with a derivation of the $K3×K3$ flux potential, which closely follows the generic Calabi-Yau derivation of [ref] .

    F-Theory and the Landscape of Intersecting D7-Branes · Threefold cycles, obstructions and the intersection matrix · 0.83

  • We begin our analysis in Section 2 with a derivation of the $K3×K3$ flux potential, which closely follows the generic Calabi-Yau derivation of [ref] .

    Fixing D7 Brane Positions by F-Theory Fluxes · Introduction · 0.86

Compares with it 3 papers
Cites it as support 3 papers
Cites it as background 17 papers
  • In the following we briefly review the dimensional reduction of eleven-dimensional supergravity on a Calabi-Yau fourfold $Y_4$ including $G_4$-flux [ref] .

    Chiral anomalies on a circle and their cancellation in F-theory · M-theory reduction with $G_4$-flux · 0.84

  • In this case they assume the standard form (see for example [ref] ) [equation] The first two conditions say that the $G_4$ is a (2,2)-form, while the last one implies $G_4$ is primitive.

    Fixing D7 Brane Positions by F-Theory Fluxes · The Potential in Terms of $W$ and $W̌$ · 0.80

  • F-Theory models with flux can be described as a limit of M-Theory compactifications on Calabi-Yau fourfolds, where the effect of a flux $G$ on the geometry is captured by the superpotentials [ref] [equation] The stationary points are characterized by $D_I W = D_k W̃ = 0$, where $I=1,…, h^3,1(X)$ and $k=1,…, h^1,1(X)$, which implies [equation] so that $G ∈H^2,2(X) ⊕H^4,0(X)$.

    More on $G$-flux and General Hodge Cycles on the Fermat Sextic · Introduction · 0.90

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