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The Super D9-Brane and its Truncations
High Energy Physics - Theory · Submitted 13 Jan 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Both of them lead to an N=1 nonlinear supersymmetrization of the D=10 cosmological constant.
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The abstract, sentence by sentence
We consider two inequivalent truncations of the super D9--brane: the ``Heterotic'' and the ``Type I'' truncation. Both of them lead to an N=1 nonlinear supersymmetrization of the D=10 cosmological constant. The propagating degrees of freedom in the Heterotic and Type I truncation are given by the components of a D=10 vector multiplet and a single Majorana-Weyl spinor, respectively. As a by-product we find that, after the Type I truncation, the Ramond-Ramond super ten-form provides an interesting reformulation of the Volkov-Akulov action. These results can be extended to all dimensions in which spacetime filling D-branes exist, i.e. D=3,4,6 and 10.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider two inequivalent truncations of the super D9--brane: the ``Heterotic'' and the ``Type I'' truncation. | contribution 0.99 | 0.82 | 0.09 | asserted 0.95 |
| s1 | Both of them lead to an N=1 nonlinear supersymmetrization of the D=10 cosmological constant. | result 1.00 | 0.78 | 0.40 | asserted 1.00 |
| s2 | The propagating degrees of freedom in the Heterotic and Type I truncation are given by the components of a D=10 vector multiplet and a single Majorana-Weyl spinor, respectively. | result 1.00 | 0.75 | 0.19 | asserted 1.00 |
| s3 | As a by-product we find that, after the Type I truncation, the Ramond-Ramond super ten-form provides an interesting reformulation of the Volkov-Akulov action. | result 0.95 | 0.93 | 0.14 | asserted 1.00 |
| s4 | These results can be extended to all dimensions in which spacetime filling D-branes exist, i.e. D=3,4,6 and 10. | result 0.63 | 0.78 | 0.18 | asserted 0.89 |
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Original abstract
We consider two inequivalent truncations of the super D9--brane: the ``Heterotic'' and the ``Type I'' truncation. Both of them lead to an N=1 nonlinear supersymmetrization of the D=10 cosmological constant. The propagating degrees of freedom in the Heterotic and Type I truncation are given by the components of a D=10 vector multiplet and a single Majorana-Weyl spinor, respectively. As a by-product we find that, after the Type I truncation, the Ramond-Ramond super ten-form provides an interesting reformulation of the Volkov-Akulov action. These results can be extended to all dimensions in which spacetime filling D-branes exist, i.e. D=3,4,6 and 10.
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References
How the literature uses it
8 arXiv papers cite this in 8 sentences
Papers citing it · 6 sentences without a confident label
Cites it as support 1 paper
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Such a potential must exist because of T-duality, and is known to couple to the D9-branes [ref] and is required for its action to be kappa-symmetric.[As in the IIA case, more potentials than this can be defined, however they generally are not required for our purposes, though we do briefly consider a 10-form potential $B^(10)$ which should presumably appear in one of our 9-form charges.
Topological BPS charges in 10 and 11-dimensional supergravity · Field equations in IIB Supergravity · 0.96
Cites it as background 1 paper
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A partially “democratic” formulation of these theories, where all the RR fields are introduced together with their magnetic duals, was given in [ref] and [ref] .
IIA/IIB Supergravity and Ten-forms · Introduction · 0.95
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