A 10-form Gauge Potential and an M-9-brane Wess-Zumino Action in Massive 11D Theory

Takeshi Sato

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A 10-form Gauge Potential and an M-9-brane Wess-Zumino Action in Massive 11D Theory

Takeshi Sato

High Energy Physics - Theory · Submitted 4 Dec 1999

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

The authors' main claim A 10-form gauge potential is consistently introduced into the massive 11D supergravity, and an M-9-brane Wess-Zumino action is constructed as that of a gauged $\sigma$-model.

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arXiv listing abstract v2. Results and the main claim are underlined; show every role.

We discuss some properties of an M-9-brane in ``massive 11D theory'' proposed by Bergshoeff, Lozano and Ortin. A 10-form gauge potential is consistently introduced into the massive 11D supergravity, and an M-9-brane Wess-Zumino action is constructed as that of a gauged $\sigma$-model. Using duality relations is crucial in deriving the action, which we learn from the study of a 9-form potential in 10D massive IIA theory. A target space solution of an M-9-brane with a non-vanishing 10-form gauge field is also obtained, whose source is shown to be the M-9-brane effective action.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#	sentence	role	the authors' own work	states the main conclusion	strength
s0	We discuss some properties of an M-9-brane in ``massive 11D theory'' proposed by Bergshoeff, Lozano and Ortin.	background 0.63	0.49	0.06	asserted 0.83
s1	A 10-form gauge potential is consistently introduced into the massive 11D supergravity, and an M-9-brane Wess-Zumino action is constructed as that of a gauged $\sigma$-model.	contribution 0.94	0.92	0.58	asserted 1.00
s2	Using duality relations is crucial in deriving the action, which we learn from the study of a 9-form potential in 10D massive IIA theory.	method 0.98	0.57	0.09	asserted 1.00
s3	A target space solution of an M-9-brane with a non-vanishing 10-form gauge field is also obtained, whose source is shown to be the M-9-brane effective action.	result 0.98	0.92	0.25	asserted 1.00

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The paper

Original abstract

We discuss some properties of an M-9-brane in ``massive 11D theory'' proposed by Bergshoeff, Lozano and Ortin. A 10-form gauge potential is consistently introduced into the massive 11D supergravity, and an M-9-brane Wess-Zumino action is constructed as that of a gauged $\sigma$-model. Using duality relations is crucial in deriving the action, which we learn from the study of a 9-form potential in 10D massive IIA theory. A target space solution of an M-9-brane with a non-vanishing 10-form gauge field is also obtained, whose source is shown to be the M-9-brane effective action.

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2 arXiv papers cite this in 8 sentences

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After multiplying by a factor of $-4R̂^-1$ one obtains: [equation] Here we consider $α̂$ as a potential to a field strength $dα̂=Ĝ^(2)$ as done explicitly in [ref] .

Topological BPS charges in 10 and 11-dimensional supergravity · 11 dimensional KK-monopole charge · 0.85

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