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New Compactifications of Eleven Dimensional Supergravity
High Energy Physics - Theory · Submitted 7 May 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim As a result, we find a new compactifying solution of the type AdS_5\times CP^3, where CP^3 is stretched along its S^2 fiber.
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The abstract, sentence by sentence
Using canonical forms on S^7, viewed as an SU(2) bundle over S^4, we introduce consistent ansatze for the 4-form field strength of eleven-dimensional supergravity and rederive the known squashed, stretched, and the Englert solutions. Further, by rewriting the metric of S^7 as a U(1) bundle over CP^3, we present yet more general ansatze. As a result, we find a new compactifying solution of the type AdS_5\times CP^3, where CP^3 is stretched along its S^2 fiber. We also find a new solution of AdS_2\times H^2\times S^7 type in Euclidean space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Using canonical forms on S^7, viewed as an SU(2) bundle over S^4, we introduce consistent ansatze for the 4-form field strength of eleven-dimensional supergravity and rederive the known squashed, stretched, and the Englert solutions. | method 0.64 | 0.93 | 0.11 | asserted 1.00 |
| s1 | Further, by rewriting the metric of S^7 as a U(1) bundle over CP^3, we present yet more general ansatze. | method 0.75 | 0.94 | 0.05 | asserted 1.00 |
| s2 | As a result, we find a new compactifying solution of the type AdS_5\times CP^3, where CP^3 is stretched along its S^2 fiber. | result 0.99 | 0.97 | 0.55 | asserted 1.00 |
| s3 | We also find a new solution of AdS_2\times H^2\times S^7 type in Euclidean space. | result 0.99 | 0.96 | 0.12 | asserted 1.00 |
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The paper
Original abstract
Using canonical forms on S^7, viewed as an SU(2) bundle over S^4, we introduce consistent ansatze for the 4-form field strength of eleven-dimensional supergravity and rederive the known squashed, stretched, and the Englert solutions. Further, by rewriting the metric of S^7 as a U(1) bundle over CP^3, we present yet more general ansatze. As a result, we find a new compactifying solution of the type AdS_5\times CP^3, where CP^3 is stretched along its S^2 fiber. We also find a new solution of AdS_2\times H^2\times S^7 type in Euclidean space.
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How the literature uses it
3 arXiv papers cite this in 10 sentences
Papers citing it · 7 sentences without a confident label
Builds on it 1 paper
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In this note, we extend the construction of [ref] to the case of compact manifold $N(1,1)$, and use the twistor space language to describe it as $U(1)$ bundle over a base which itself is an $S^2$ bundle on $CP^2$; the flag manifold.
Type IIB flux compactifications on twistor bundles · Introduction · 1.00
Uses its method or tool 1 paper
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As in [ref] , it also proves useful to define the following self-dual 2-forms R_1 = sin_1 (e^01+e^23) -cos_1(e^02+e^31) , R_2 = cosþ_1cos_1 (e^01+e^23)+ cosþ_1 sin_1 (e^02+e^31)-sinþ_1 (e^03+e^12) , K = sinþ_1cos_1 (e^01+e^23)+ sinþ_1 sin_1 (e^02+e^31)+cosþ_1 (e^03+e^12) , where we have used the shorthand notation $e^ij=e^ie^j$.
An $S^3\times S^3$ bundle over $S^4$ and new supergravity solutions · The ansatz for $F_4$ · 0.98
What it cites · 3 sentences without a confident label
Cites as background 1 paper
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It is also worth studying the new solutions in the context of holographic superconductivity in M-theory [ref] .
Quantum Criticality and Holographic Superconductors in M-theory · Conclusions · 0.81
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