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Brane Descent Relations in M-theory
High Energy Physics - Theory · Submitted 25 Jan 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We discuss how the BPS branes of M-theory could be described as bound states of non-BPS M10-branes.
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We discuss how the BPS branes of M-theory could be described as bound states of non-BPS M10-branes. This conjectured M10-brane is constructed as an unstable spacetime-filling brane in the massive eleven dimensional supergravity defined with a Killing direction, such that 1) the BPS M9-brane is obtained after the tachyonic mode of an M2-brane ending on it condenses, and 2) it gives the non-BPS D9-brane of the type IIA theory upon reduction. The existence of other non-BPS M-branes is also discussed, together with their possible stabilisation within the Horava-Witten construction.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss how the BPS branes of M-theory could be described as bound states of non-BPS M10-branes. | contribution 0.98 | 0.56 | 0.46 | hedged possibility 1.00 |
| s1 | This conjectured M10-brane is constructed as an unstable spacetime-filling brane in the massive eleven dimensional supergravity defined with a Killing direction, such that 1) the BPS M9-brane is obtained after the tachyonic mode of an M2-brane ending on it condenses, and 2) it gives the non-BPS D9-brane of the type IIA theory upon reduction. | contribution 0.87 | 0.52 | 0.35 | speculative 0.63 |
| s2 | The existence of other non-BPS M-branes is also discussed, together with their possible stabilisation within the Horava-Witten construction. | contribution 0.96 | 0.54 | 0.08 | hedged possibility 0.70 |
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Original abstract
We discuss how the BPS branes of M-theory could be described as bound states of non-BPS M10-branes. This conjectured M10-brane is constructed as an unstable spacetime-filling brane in the massive eleven dimensional supergravity defined with a Killing direction, such that 1) the BPS M9-brane is obtained after the tachyonic mode of an M2-brane ending on it condenses, and 2) it gives the non-BPS D9-brane of the type IIA theory upon reduction. The existence of other non-BPS M-branes is also discussed, together with their possible stabilisation within the Horava-Witten construction.
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