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Exact Embedding of N=1, D=7 Gauged Supergravity in D=11
High Energy Physics - Theory · Submitted 22 Jun 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We obtain the explicit and complete bosonic non-linear Kaluza-Klein ansatz for the consistent S^4 reduction of D=11 supergravity to N=1, D=7 gauged supergravity.
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The abstract, sentence by sentence
We obtain the explicit and complete bosonic non-linear Kaluza-Klein ansatz for the consistent S^4 reduction of D=11 supergravity to N=1, D=7 gauged supergravity. This provides a geometrical interpretation of the lower dimensional solutions from the eleven-dimensional point of view.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We obtain the explicit and complete bosonic non-linear Kaluza-Klein ansatz for the consistent S^4 reduction of D=11 supergravity to N=1, D=7 gauged supergravity. | contribution 0.58 | 0.96 | 0.88 | asserted 1.00 |
| s1 | This provides a geometrical interpretation of the lower dimensional solutions from the eleven-dimensional point of view. | interpretation 1.00 | 0.64 | 0.15 | asserted 1.00 |
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The paper
Original abstract
We obtain the explicit and complete bosonic non-linear Kaluza-Klein ansatz for the consistent S^4 reduction of D=11 supergravity to N=1, D=7 gauged supergravity. This provides a geometrical interpretation of the lower dimensional solutions from the eleven-dimensional point of view.
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References
How the literature uses it
19 arXiv papers cite this in 43 sentences
Papers citing it · 25 sentences without a confident label
Builds on it 1 paper
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We will give an extension to the result of [ref] by constructing $SO(4)$ gauged theory including topological mass term from a truncation of $S^4$ reduction of eleven dimensional supergravity.
N=2 SO(4) 7D gauged supergravity with topological mass term from 11 dimensions · Introduction · 0.99
Uses its method or tool 3 papers
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The 11d truncation Ansatz takes then the simplified form [ref] [equation] where, for simplicty of notation, $s=sinξ$ and $c=cosξ$.
Searching for Coleman-de Luccia bubbles in AdS compactifications · Supergravity setup and AdS$_7$ vacua · 0.84
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We present the explicit 11d geometry obtained by using the uplift formulas in [ref] , to then show that it belongs to the general classification of AdS$_3×S^3 ×S^3 ×Σ_2$ solutions to M-theory of [ref] , preserving large $N=(4,4)$ supersymmetry.
Half-BPS Janus solutions in AdS$_7$ · The Janus solution in M-theory · 0.88
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To obtain the topological mass term, we will impose the so-called odd-dimensional self-duality as in [ref] .
N=2 SO(4) 7D gauged supergravity with topological mass term from 11 dimensions · Seven dimensional $N=2$ gauged supergravity from eleven dimensions · 0.94
Compares with it 2 papers
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The above potential becomes [equation] which is exactly the same as that given in [ref] up to a redefinition of the coupling constant $g$.
N=2 SO(4) 7D gauged supergravity with topological mass term from 11 dimensions · $SO(4)$ $N=2$ gauged supergravity from $S^4$ reduction · 1.00
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When comparing our truncation ansatz with the one given in Section 4.1 of [ref] , one should take into account that $Â^here=-Â^FNR$ (this is seen from comparing our 11d Maxwell equation with the one in [ref] , which provides the 7d to 11d uplift formulae used in [ref] ).
$\mathcal{N}=2$ consistent truncations from wrapped M5-branes · The truncation ansatz · 0.98
Cites it as background 8 papers
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It is well known that the equations of motion of the minimal gauged supergravity in $d=7$ written in [ref] are obtained by reducing eleven-dimensional supergravity on $S^4$ [ref] .
Supersymmetric objects in gauged supergravities · BPS Objects in $d=7$ and their M-Theory Origin · 0.82
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It is well-known that M-theory can be consistently reduced over 4-spheres (see e.g. [ref] ).
Searching for Coleman-de Luccia bubbles in AdS compactifications · Supergravity setup and AdS$_7$ vacua · 0.96
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However, there are many subtleties involved with sphere truncations (see e.g. [ref] ) and more general coset reductions (see e.g. [ref] ).
Rounding out the story of higher derivative consistent truncations · Introduction and summary · 0.98
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