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Supergravity couplings: a geometric formulation

High Energy Physics - Theory · Submitted 24 May 2000

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

The authors' main claim At a more advanced level this approach is generalized to include tensor field and Chern-Simons couplings in supersymmetry and supergravity, relevant in the context of weakly and strongly coupled string theories.

how it is stated · asserted 0.99 read the record →

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arXiv IDhep-th/0005225 (version 1)
Pith IDEHIEQQWJ, Pith's permanent record of this paper and its review
CitationG. Girardi, P. Binetruy, R. Grimm. "Supergravity couplings: a geometric formulation." arXiv:hep-th/0005225 (2000). https://pith.science/paper/EHIEQQWJ
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What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.09 · human participants 0.01 · controlled comparison 0.01 · randomized assignment 0.01 · states quantitative result 0.02 · compares with prior results 0.06 · mentions code or data availability 0.02.

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

This report provides a pedagogical introduction to the description of the general Poincare supergravity/matter/Yang-Mills couplings using methods of Kahler superspace geometry. At a more advanced level this approach is generalized to include tensor field and Chern-Simons couplings in supersymmetry and supergravity, relevant in the context of weakly and strongly coupled string theories.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 This report provides a pedagogical introduction to the description of the general Poincare supergravity/matter/Yang-Mills couplings using methods of Kahler superspace geometry. contribution 0.97 0.46 0.13 asserted 0.99
s1 At a more advanced level this approach is generalized to include tensor field and Chern-Simons couplings in supersymmetry and supergravity, relevant in the context of weakly and strongly coupled string theories. contribution 0.95 0.47 0.15 asserted 0.99

What kind of paper the classifier reports this is: review 0.71 · evidence from proof or derivation 0.76.

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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

This report provides a pedagogical introduction to the description of the general Poincare supergravity/matter/Yang-Mills couplings using methods of Kahler superspace geometry. At a more advanced level this approach is generalized to include tensor field and Chern-Simons couplings in supersymmetry and supergravity, relevant in the context of weakly and strongly coupled string theories.

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References
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35 arXiv papers cite this in 70 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 · 41 sentences without a confident label

Builds on it 2 papers
Uses its method or tool 4 papers
  • [ref], where the Kähler metric is derived from $K$, see [ref] .

    Classification of Shift-Symmetric No-Scale Supergravities · Duality Transformation · 0.84

  • In the $U(1)_K$ superspace formalism [ref] , the kinetic contribution to the effective supergravity action is determined by the superspace integral [equation] where $E$ is the supervielbein determinant.

    Heterotic de Sitter Beyond Modular Symmetry · Stringy de Sitter Vacua & the Linear Multiplet Formalism · 0.89

  • Following [ref] and [ref] , one chooses $H$ to obey the constraints [equation] Then as a consequence of the Bianchi identities, one can show that [equation] where $L$ is a linear superfield and where we have defined [equation] It follows that the dual of the three form is [equation]

    N=1 Conformal Superspace in Four Dimensions · New minimal supergravity · 0.89

Compares with it 1 paper
  • Using [equation] one finds [equation] This is equivalent to the corresponding formulae in equations (B-2.12) through (B-2.18) of [ref] ; therefore, the torsion of $U(1)$ supergravity is equivalent to the $B=0$ gauge of conformal superspace.

    N=1 Conformal Superspace in Four Dimensions · Some consistency checks · 1.00

Cites it as support 1 paper
Cites it as background 14 papers
  • To simplify the discussion, let us first assume that the only low energy degrees of freedom are the gravity multiplet, chiral multiplets $S,$ and the linear multiplet $L.$ The two-derivative action of linear multiplets are determined by two functions $F$ and $K$ [ref] [equation] where $E$ is the super-vielbein, the function $F$ depends on the Kähler potential $K(S,S̅,L)$ via the constraint [equation] which is imposed to obtain the correct normalization of the Einstein-Hilbert action in Einstein-frame.

    On one-loop corrected dilaton action in string theory · Effective action in linear multiplet formalism · 0.86

  • Recall that this action arose by performing a duality transformation on the action [equation] There exists a quite elegant formulation for dealing with this model, known as Kähler superspace, which was constructed originally in [ref] .[See [ref] for a recent detailed and pedagogical discussion.] As a first step toward understanding how to geometrize the dual action, we will describe how Kähler superspace arises via the compensator method.

    A dual formulation of supergravity-matter theories · The geometry of matter couplings in non-minimal supergravity · 0.80

  • In $N=1$ supersymmetric theories the massless 3-form resides in a supermultiplet together with two scalar and two fermionic physical degrees of freedom [ref] and Poincaré duality relates this multiplet to a non-minimal scalar multiplet discussed in [ref] .[ Since 3-forms can also play the role of the Yang-Mills Chern-Simons term, the 3-form multiplet has been used in the description of gauge anomalies in supersymmetric theories [ref] .] A massive 3-form multiplet gains its mass by “eating” a linear multiplet which contains a 2-form as one of its components.

    Duality and Couplings of 3-Form-Multiplets in N=1 Supersymmetry · Introduction · 0.85

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