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(Twisted) Toroidal Compactification of pp-Waves
High Energy Physics - Theory · Submitted 15 Mar 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim $T^2$ compactifications can preserve 20, 18 or 16 supercharges; $T^3$ compactifications can preserve 18 or 16 supercharges and higher compactifications preserve 16 supercharges.
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The abstract, sentence by sentence
The maximally supersymmetric type IIB pp-wave is compactified on spatial circles, with and without an auxiliary rotational twist. All spatial circles of constant radius are identified. Without the twist, an S$^1$ compactification can preserve 24, 20 or 16 supercharges. $T^2$ compactifications can preserve 20, 18 or 16 supercharges; $T^3$ compactifications can preserve 18 or 16 supercharges and higher compactifications preserve 16 supercharges. The worldsheet theory of this background is discussed. The T-dual and decompactified type IIA and M-theoretic solutions which preserve 24 supercharges are given. Some comments are made regarding the AdS parent and the CFT description.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The maximally supersymmetric type IIB pp-wave is compactified on spatial circles, with and without an auxiliary rotational twist. | contribution 0.85 | 0.81 | 0.10 | asserted 0.99 |
| s1 | All spatial circles of constant radius are identified. | method 0.81 | 0.56 | 0.04 | asserted 1.00 |
| s2 | Without the twist, an S$^1$ compactification can preserve 24, 20 or 16 supercharges. | result 1.00 | 0.78 | 0.20 | asserted 0.72 |
| s3 | $T^2$ compactifications can preserve 20, 18 or 16 supercharges; $T^3$ compactifications can preserve 18 or 16 supercharges and higher compactifications preserve 16 supercharges. | result 1.00 | 0.80 | 0.22 | asserted 0.70 |
| s4 | The worldsheet theory of this background is discussed. | contribution 0.96 | 0.81 | 0.04 | asserted 0.92 |
| s5 | The T-dual and decompactified type IIA and M-theoretic solutions which preserve 24 supercharges are given. | result 0.64 | 0.86 | 0.14 | asserted 1.00 |
| s6 | Some comments are made regarding the AdS parent and the CFT description. | interpretation 0.79 | 0.71 | 0.05 | asserted 0.61 |
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Original abstract
The maximally supersymmetric type IIB pp-wave is compactified on spatial circles, with and without an auxiliary rotational twist. All spatial circles of constant radius are identified. Without the twist, an S$^1$ compactification can preserve 24, 20 or 16 supercharges. $T^2$ compactifications can preserve 20, 18 or 16 supercharges; $T^3$ compactifications can preserve 18 or 16 supercharges and higher compactifications preserve 16 supercharges. The worldsheet theory of this background is discussed. The T-dual and decompactified type IIA and M-theoretic solutions which preserve 24 supercharges are given. Some comments are made regarding the AdS parent and the CFT description.
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References
How the literature uses it
5 arXiv papers cite this in 8 sentences
Papers citing it · 6 sentences without a confident label
Builds on it 1 paper
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The string frame metric ([ref]) is now modified to [The coordinates used here make a space-like isometry explicit [ref] ] ds^2 = 2dx^+dx^- - 4μ^2[(x^1)^2+⋯(x^6)^2](dx^+)^2 - 8μx^7 dx^8 dx^+ + [(dx^1)^2 + ⋯(dx^8)^2] The dilaton remains the same as ([ref]), and there is an additional 5-form field strength F_+1234 = F_+5678 = μ e^Qx^+ For $Q=0$, the matrix membrane theory has been considered in [ref] .
Holography and Cosmological Singularities · pp-wave Big Bangs · 0.81
Cites it as background 1 paper
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We consider briefly the interplay between the decoupling limit [ref] and the Penrose limit of [ref] , which is a geometric limit of the $_5 ×S^5$ background giving the maximally supersymmetric pp-wave background of [ref] , in the coordinate system with a flat direction [ref] .
Matching gauge theory and string theory in a decoupling limit of AdS/CFT · Introduction · 0.83
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