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Consistency of Kaluza-Klein Sphere Reductions of Symmetric Potentials

High Energy Physics - Theory · Submitted 7 Feb 2000

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

The authors' main claim Here, we complete the proof, by showing explicitly that the full set of higher-dimensional equations of motion are satisfied if and only if the lower-dimensional fields satisfy the relevant scalar plus gravity equations.

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arXiv IDhep-th/0002056 (version 3)
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CitationA. Sadrzadeh, C.N. Pope, H. Lu, M. Cvetic. "Consistency of Kaluza-Klein Sphere Reductions of Symmetric Potentials." arXiv:hep-th/0002056 (2000). https://pith.science/paper/LFI7L3MW
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What the abstract itself states, as probabilities: claims first 0.08 · states limitation 0.21 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.84 · mentions code or data availability 0.02.

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arXiv listing abstract v3. Results and the main claim are underlined; .

In a recent paper, the complete (non-linear) Kaluza-Klein Ansatz for the consistent embedding of certain scalar plus gravity subsectors of gauged maximal supergravity in D=4, 5 and 7 was presented, in terms of sphere reductions from D=11 or type IIB supergravity. The scalar fields included in the truncations were the diagonal fields in the SL(N,R)/SO(N) scalar submanifolds of the full scalar sectors of the corresponding maximal supergravities, with N=8, 6 and 5. The embeddings were used for obtaining an interpretation of extremal D=4, 5 or 7 AdS domain walls in terms of distributed M-branes or D-branes in the higher dimensions. Although strong supporting evidence for the correctness of the embedding Ansatze was presented, a full proof of the consistency was not given. Here, we complete the proof, by showing explicitly that the full set of higher-dimensional equations of motion are satisfied if and only if the lower-dimensional fields satisfy the relevant scalar plus gravity equations.

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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 In a recent paper, the complete (non-linear) Kaluza-Klein Ansatz for the consistent embedding of certain scalar plus gravity subsectors of gauged maximal supergravity in D=4, 5 and 7 was presented, in terms of sphere reductions from D=11 or type IIB supergravity. background 0.98 0.09 0.06 asserted 1.00
s1 The scalar fields included in the truncations were the diagonal fields in the SL(N,R)/SO(N) scalar submanifolds of the full scalar sectors of the corresponding maximal supergravities, with N=8, 6 and 5. background 0.82 0.21 0.03 asserted 1.00
s2 The embeddings were used for obtaining an interpretation of extremal D=4, 5 or 7 AdS domain walls in terms of distributed M-branes or D-branes in the higher dimensions. interpretation 0.49 0.30 0.03 asserted 1.00
s3 Although strong supporting evidence for the correctness of the embedding Ansatze was presented, a full proof of the consistency was not given. gap 0.99 0.14 0.04 asserted 0.97
s4 Here, we complete the proof, by showing explicitly that the full set of higher-dimensional equations of motion are satisfied if and only if the lower-dimensional fields satisfy the relevant scalar plus gravity equations. contribution 0.93 0.96 0.94 asserted 1.00

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

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The paper
Original abstract

In a recent paper, the complete (non-linear) Kaluza-Klein Ansatz for the consistent embedding of certain scalar plus gravity subsectors of gauged maximal supergravity in D=4, 5 and 7 was presented, in terms of sphere reductions from D=11 or type IIB supergravity. The scalar fields included in the truncations were the diagonal fields in the SL(N,R)/SO(N) scalar submanifolds of the full scalar sectors of the corresponding maximal supergravities, with N=8, 6 and 5. The embeddings were used for obtaining an interpretation of extremal D=4, 5 or 7 AdS domain walls in terms of distributed M-branes or D-branes in the higher dimensions. Although strong supporting evidence for the correctness of the embedding Ansatze was presented, a full proof of the consistency was not given. Here, we complete the proof, by showing explicitly that the full set of higher-dimensional equations of motion are satisfied if and only if the lower-dimensional fields satisfy the relevant scalar plus gravity equations.

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7 arXiv papers cite this in 11 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

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  • More concretely, we started by using the fact that a dimensional reduction of Type IIB supergravity along the $S^5$ yields 5D $=8$ gauged supergravity [ref] , which is a consistent reduction of the full Type IIB supergravity on AdS$_5×S^5$ [ref] (the full non-linear reduction ansatzë for the AdS$_5×S^5$ compactification of IIB supergravity was worked out in [ref] ).

    Charged Rotating Hairy Black Holes in AdS$_5 \times S^5$: Unveiling their Secrets · Summary and Comments · 0.88

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