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M5 brane from mass deformed BLG theory

High Energy Physics - Theory · Submitted 14 Sep 2009

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

The authors' main claim We realize the BLG theory by a Nambu bracket and find a maximally supersymmetric lagrangian for the fluctuation fields corresponding to a single M5 brane on $\mb{R}^{1,2}\times S^3$.

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arXiv ID0909.2518 (version 3)
Pith ID6WLJIPLF, Pith's permanent record of this paper and its review
CitationAndreas Gustavsson. "M5 brane from mass deformed BLG theory." arXiv:0909.2518 (2009). https://pith.science/paper/6WLJIPLF
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What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.07 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.06 · mentions code or data availability 0.02.

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

We study small fluctuations around a BPS three-sphere vacuum solution of mass deformed BLG theory. We realize the BLG theory by a Nambu bracket and find a maximally supersymmetric lagrangian for the fluctuation fields corresponding to a single M5 brane on $\mb{R}^{1,2}\times S^3$.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We study small fluctuations around a BPS three-sphere vacuum solution of mass deformed BLG theory. contribution 0.96 0.92 0.08 asserted 0.92
s1 We realize the BLG theory by a Nambu bracket and find a maximally supersymmetric lagrangian for the fluctuation fields corresponding to a single M5 brane on $\mb{R}^{1,2}\times S^3$. contribution 0.48 0.95 0.69 asserted 1.00

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We study small fluctuations around a BPS three-sphere vacuum solution of mass deformed BLG theory. We realize the BLG theory by a Nambu bracket and find a maximally supersymmetric lagrangian for the fluctuation fields corresponding to a single M5 brane on $\mb{R}^{1,2}\times S^3$.

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References
How the literature uses it

7 arXiv papers cite this in 10 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

Papers citing it · 4 sentences without a confident label

Contests it 1 paper
  • We list these terms below, expanded around the vacuum to quadratic order (more details on this computation are found in [ref] , though there is some crucial sign error in this work), Ł_pot = - 1/2 (D_αY^α)^2 - 1/R^2 Y^α Y_α + \(3/2 - 3^2\) \(Y/R\)^2 - 6 Y/R D_α Y^α - 1/2 g^αβ ∂_α Y ∂_β Y - 1/2R^2 Y^α Y_α Ł_flux = 4 Y/R D_αY^α + 6 \(Y/R\)^2 + 2/R^2 Y^αY_α Ł_m = -1/2R^2 Y^α Y_α - 1/2 \(Y/R\)^2 Summing these contributions we get the following contribution from the mass-deformed sextic potential Ł_mpot = -1/2 (D_αY^α)^2 - 2 Y/R D_αY^α - 2 \(Y/R\)^2 - 1/2 g^αβ ∂_α Y ∂_β Y In particular we see that the mass term for $Y^α$ vanishes by a fortunate cancelation.

    M5 brane on $R^{1,2} \times S^3$ · Deconstructing M5 brane Lagrangian · contest 0.94

Cites it as background 5 papers
  • Starting from the BLG model, an action for M5-brane was constructed in Ho-Matsuo [ref] and Ho-Imamura-Matsuo-Shiba [ref] by taking the Lie 3-algebra which is defined through the Nambu-bracket [ref] .[ Also see Ref. [ref] for a similar construction of M5-brane action in a different background.] This is in parallel with the construction of a D$p$-brane in a constant $B$-field background from infinitely many D($p-2$)-branes [ref] .

    Non-Linearly Extended Self-Dual Relations From The Nambu-Bracket Description Of M5-Brane In A Constant C-Field Background · Introduction · 0.91

  • In another line of development, BPS configurations of the BLG theory have been studied leading to their classification based on R-symmetry breaking [ref] , following a similar classification in Yang-Mills theories [ref] .

    Moduli and BPS configurations of the BLG theory · Introduction · 0.92

  • It is possible to break the Lorentz symmetry down to the $SIM(1)$ symmetry by adding a suitable mass term [ref] [equation] It may be noted that the mass deformed BLG theory is thought to be related to the theory of M5-branes [ref] .

    Chern-Simons Theory in SIM(1) Superspace · Chern-Simons Theory with $SIM(1)$ Projections · 0.87

What it cites · 33 sentences without a confident label

Uses the method or tool of 2 papers
Compares with 1 paper
  • Since many calculations in our paper are the same as those in [ref] , we should contrast those calculations with ours.

    M5 from M2 · Fluctuation analysis · 0.99

Cites as background 9 papers

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