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F-Theory GUT Vacua on Compact Calabi-Yau Fourfolds

High Energy Physics - Theory · Submitted 18 Dec 2009

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

The authors' main claim We present compact three-generation F-theory GUT models meeting in particular the constraints of D3-tadpole cancellation and D-term supersymmetry.

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arXiv ID0912.3524 (version 2)
Pith IDNIRBY5FG, Pith's permanent record of this paper and its review
CitationSven Krause, Thomas W. Grimm, Timo Weigand. "F-Theory GUT Vacua on Compact Calabi-Yau Fourfolds." arXiv:0912.3524 (2009). https://pith.science/paper/NIRBY5FG
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.16 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.61 · compares with prior results 0.06 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

We present compact three-generation F-theory GUT models meeting in particular the constraints of D3-tadpole cancellation and D-term supersymmetry. To this end we explicitly construct elliptically fibered Calabi-Yau fourfolds as complete intersections in a toric ambient space. Toric methods enable us to control the singular geometry of the SU(5) GUT model. The GUT brane wraps a non-generic del Pezzo surface admitting GUT symmetry breaking via hypercharge flux. It is contractible to a curve and we demonstrate the existence of a consistent decoupling limit. We compute the Euler characteristic of the singular Calabi-Yau fourfold to show that our three-generation flux solutions obtained via the spectral cover construction are consistent with D3-tadpole cancellation.

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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 present compact three-generation F-theory GUT models meeting in particular the constraints of D3-tadpole cancellation and D-term supersymmetry. contribution 0.96 0.95 0.75 asserted 1.00
s1 To this end we explicitly construct elliptically fibered Calabi-Yau fourfolds as complete intersections in a toric ambient space. method 0.92 0.95 0.06 asserted 1.00
s2 Toric methods enable us to control the singular geometry of the SU(5) GUT model. method 0.93 0.66 0.04 asserted 1.00
s3 The GUT brane wraps a non-generic del Pezzo surface admitting GUT symmetry breaking via hypercharge flux. contribution 0.64 0.78 0.10 asserted 1.00
s4 It is contractible to a curve and we demonstrate the existence of a consistent decoupling limit. result 0.79 0.91 0.08 asserted 1.00
s5 We compute the Euler characteristic of the singular Calabi-Yau fourfold to show that our three-generation flux solutions obtained via the spectral cover construction are consistent with D3-tadpole cancellation. result 0.81 0.96 0.28 asserted 0.94

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.97.

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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 present compact three-generation F-theory GUT models meeting in particular the constraints of D3-tadpole cancellation and D-term supersymmetry. To this end we explicitly construct elliptically fibered Calabi-Yau fourfolds as complete intersections in a toric ambient space. Toric methods enable us to control the singular geometry of the SU(5) GUT model. The GUT brane wraps a non-generic del Pezzo surface admitting GUT symmetry breaking via hypercharge flux. It is contractible to a curve and we demonstrate the existence of a consistent decoupling limit. We compute the Euler characteristic of the singular Calabi-Yau fourfold to show that our three-generation flux solutions obtained via the spectral cover construction are consistent with D3-tadpole cancellation.

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How the literature uses it

68 arXiv papers cite this in 137 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 · 79 sentences without a confident label

Builds on it 2 papers
Uses its method or tool 7 papers
  • Following [ref] we will blow up points and curves inside the Fano threefolds until the requirements for a GUT model are satisfied.

    Global SO(10) F-theory GUTs · General idea · 0.81

  • The gauge theory will be $SU(5)$ and $SU(5) ×U(1)$ and we perform an explicit resolution of all co-dimension singularities as in [ref] by modifying the toric ambient space.

    F-theory fluxes, Chirality and Chern-Simons theories · Introduction · 0.97

  • A useful indirect procedure to determine such components has been established, through the matching of Chern-Simons (CS) terms in M/F-theory duality [ref] .

    Applications of Flux Compactifications in F-Theory · Chiral matter and matter surfaces · 0.96

Compares with it 2 papers
Cites it as support 3 papers
Cites it as background 37 papers

What it cites · 97 sentences without a confident label

Builds on 1 paper
  • To remedy this problem, we generalise the geometries of [ref] to an entire sequence of torically constructed Calabi-Yau fourfolds.

    Global F-theory GUTs · Introduction · 1.00

Uses the method or tool of 9 papers
  • It is not hard to check that the splits of $∇$ into $(∇_1,∇_2)$ determine a valid nef-partition.[This can be done by using the program PALP [ref] .] Since $∇_1$ contains the points $(ν_1,ν_2,ν_3)$ corresponding to the coordinates $(x,y,z)$ of the elliptic fiber one checks using [ref] that $p_1 ≡P_W=0$ is precisely the Tate form [ref].

    math/0204356 · On the toric construction of elliptic fourfolds · 1.00

  • E.g. the computation of the relevant Euler characteristic, either directly [ref] or via the method proposed for a certain class of geometries in [ref] , requires explicit control of the singularities of $Y$.

    Global F-theory GUTs · Calabi-Yau fourfolds in toric ambient spaces · 0.83

  • E.g. the computation of the relevant Euler characteristic, either directly [ref] or via the method proposed for a certain class of geometries in [ref] , requires explicit control of the singularities of $Y$.

    From Local to Global in F-Theory Model Building · Calabi-Yau fourfolds in toric ambient spaces · 0.83

Uses data or values from 1 paper
  • Here we merely list the final results from [ref] in terms of the above parametrisation of the spectral cover line bundle,

    Global F-theory GUTs · Gauge flux from spectral cover bundles · 0.82

Compares with 1 paper
  • In the compact examples of the type discussed in [ref] and in this article, by contrast, $S$ is a non-generic del Pezzo surface and is only contractible to a curve.

    Global F-theory GUTs · Decoupling Limit · 0.87

Cites as support 1 paper
  • Indeed, the above choice guarantees that $c_1(V) + c_1(L) =0$ [ref] .

    Global F-theory GUTs · Gauge flux from spectral cover bundles · 0.97

Cites as background 36 papers
  • It is interpreted as the result of breaking the maximal $E_8$ enhancement of the $ℙ_1,2,3[6]$ fiber by a non-trivial Higgs bundle [ref] with structure group $H$ over $S$.

    GUTs and Exceptional Branes in F-theory - I · Spectral covers for $SU(5)$ models · 0.87

  • It is interpreted as the result of breaking the maximal $E_8$ enhancement of the $ℙ_1,2,3[6]$ fiber by a non-trivial Higgs bundle [ref] with structure group $H$ over $S$.

    Model Building with F-Theory · Spectral covers for $SU(5)$ models · 0.87

  • The explicit construction of compact $SU(5)$ GUT vacua with hypercharge induced GUT symmetry breaking [ref] was initiated in [ref] actually not in fully fledged F-theory, but, as a first step, in the framework of Type IIB orientifolds within the well-defined framework of toric geometry.

    GUTs and Exceptional Branes in F-theory - II: Experimental Predictions · Introduction · 0.86

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