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A geometric formulation of exceptional field theory

High Energy Physics - Theory · Submitted 2 May 2016

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

The authors' main claim We formulate the full bosonic SL(5) exceptional field theory in a coordinate-invariant manner.

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arXiv ID1605.00385 (version 1)
Pith ID35MWRADS, Pith's permanent record of this paper and its review
CitationDieter Lust, Emanuel Malek, Falk Hassler, Pascal du Bosque. "A geometric formulation of exceptional field theory." arXiv:1605.00385 (2016). https://pith.science/paper/35MWRADS
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 3,667 input tokens.

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.28 · human participants 0.01 · controlled comparison 0.01 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.58 · mentions code or data availability 0.02.

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arXiv listing abstract v1. Results and the main claim are underlined; .

We formulate the full bosonic SL(5) exceptional field theory in a coordinate-invariant manner. Thereby we interpret the 10-dimensional extended space as a manifold with $\mathrm{SL}(5)\times\mathbb{R}^+$-structure. We show that the algebra of generalised diffeomorphisms closes subject to a set of closure constraints which are reminiscent of the quadratic and linear constraints of maximal seven-dimensional gauged supergravities, as well as the section condition. We construct an action for the full bosonic SL(5) exceptional field theory, even when the $\mathrm{SL}(5)\times\mathbb{R}^+$-structure is not locally flat.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We formulate the full bosonic SL(5) exceptional field theory in a coordinate-invariant manner. contribution 1.00 0.96 0.38 asserted 1.00
s1 Thereby we interpret the 10-dimensional extended space as a manifold with $\mathrm{SL}(5)\times\mathbb{R}^+$-structure. interpretation 0.94 0.90 0.16 asserted 1.00
s2 We show that the algebra of generalised diffeomorphisms closes subject to a set of closure constraints which are reminiscent of the quadratic and linear constraints of maximal seven-dimensional gauged supergravities, as well as the section condition. result 0.89 0.94 0.25 asserted 1.00
s3 We construct an action for the full bosonic SL(5) exceptional field theory, even when the $\mathrm{SL}(5)\times\mathbb{R}^+$-structure is not locally flat. contribution 0.96 0.96 0.26 asserted 1.00

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

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The paper
Original abstract

We formulate the full bosonic SL(5) exceptional field theory in a coordinate-invariant manner. Thereby we interpret the 10-dimensional extended space as a manifold with $\mathrm{SL}(5)\times\mathbb{R}^+$-structure. We show that the algebra of generalised diffeomorphisms closes subject to a set of closure constraints which are reminiscent of the quadratic and linear constraints of maximal seven-dimensional gauged supergravities, as well as the section condition. We construct an action for the full bosonic SL(5) exceptional field theory, even when the $\mathrm{SL}(5)\times\mathbb{R}^+$-structure is not locally flat.

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References
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9 arXiv papers cite this in 27 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 · 18 sentences without a confident label

Builds on it 1 paper
Uses its method or tool 1 paper
Compares with it 2 papers
Cites it as background 2 papers

What it cites · 88 sentences without a confident label

Builds on 8 papers
Uses the method or tool of 7 papers
  • We will use a Weitzenböck-like connection [equation] and derive $V_1$ in terms of the generalised torsion of this connection, mirroring the construction in [ref] .[This is related to the flux formulation of DFT and EFT but is different to the construction used in [ref] .] The generalised torsion is defined as [equation] where $_ab$ is an irrep of the generalised torsion.

    The O_{D,D} Geometry of String Theory · Scalar potential · 0.80

  • We will use a Weitzenböck-like connection [equation] and derive $V_1$ in terms of the generalised torsion of this connection, mirroring the construction in [ref] .[This is related to the flux formulation of DFT and EFT but is different to the construction used in [ref] .] The generalised torsion is defined as [equation] where $_ab$ is an irrep of the generalised torsion.

    Geometry and fluxes of SL(5) exceptional field theory · Scalar potential · 0.80

  • We will use a Weitzenböck-like connection [equation] and derive $V_1$ in terms of the generalised torsion of this connection, mirroring the construction in [ref] .[This is related to the flux formulation of DFT and EFT but is different to the construction used in [ref] .] The generalised torsion is defined as [equation] where $_ab$ is an irrep of the generalised torsion.

    Flux Formulation of DFT on Group Manifolds and Generalized Scherk-Schwarz Compactifications · Scalar potential · 0.80

Compares with 12 papers
  • The first two lines in [ref] reduce immediately to the $$ EFT action of [ref] when the covariant derivatives are replaced by partial derivatives, while the final line represents a non-minimal modification in the case of fluxes, just as in $$ [ref] .

    Exceptional field theory: $SL(5)$ · Scalar potential · 1.00

  • The first two lines in [ref] reduce immediately to the $$ EFT action of [ref] when the covariant derivatives are replaced by partial derivatives, while the final line represents a non-minimal modification in the case of fluxes, just as in $$ [ref] .

    Double Field Theory on Group Manifolds · Scalar potential · 1.00

  • The first two lines in [ref] reduce immediately to the $$ EFT action of [ref] when the covariant derivatives are replaced by partial derivatives, while the final line represents a non-minimal modification in the case of fluxes, just as in $$ [ref] .

    Generalized Metric Formulation of Double Field Theory on Group Manifolds · Scalar potential · 1.00

Cites as support 1 paper
Cites as background 24 papers
  • Apart from the potential, the various terms appearing in the action [ref] are very similar to the usual EFT construction, see for example the original discussion in [ref] and the specific example of $$ in [ref] , and so we will keep their discussion brief.

    Exceptional field theory: $SL(5)$ · The action · 0.90

  • Apart from the potential, the various terms appearing in the action [ref] are very similar to the usual EFT construction, see for example the original discussion in [ref] and the specific example of $$ in [ref] , and so we will keep their discussion brief.

    Exceptional Field Theory I: $E_{6(6)}$ covariant Form of M-Theory and Type IIB · The action · 0.90

  • Double field theory (DFT) [ref] has grown out of a desire to better understand T-duality by using a formalism in which it is made manifest [ref] .

    Double Field Theory · Introduction · 0.99

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