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String theory

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v t e

In theoretical physics, an M2-brane, is a spatially extended mathematical object (brane) that appears in string theory and in related theories (e.g. M-theory, F-theory). In particular, it is a solution of eleven-dimensional supergravity which possesses a three-dimensional world volume.

Description

The M2-brane solution can be found^[1] by requiring [math]\displaystyle{ (Poincare)_{3}\times SO(8) }[/math] symmetry of the solution and solving the supergravity equations of motion with the p-brane ansatz. The solution is given by a metric and three-form gauge field which, in isotropic coordinates, can be written as

[math]\displaystyle{ \begin{align} ds^{2}_{M2} &= \left(1+\frac{q}{r^{6}}\right)^{-\frac{2}{3}}dx^{\mu} dx^{\nu}\eta_{\mu\nu} + \left(1+\frac{q}{r^{6}}\right)^{\frac{1}{3}}dx^{i}dx^{j}\delta_{ij} \\ F_{i\mu_{1}\mu_{2}\mu_{3}} &= \epsilon_{\mu_{1}\mu_{2}\mu_{3}} \partial_{i}\left(1+\frac{q}{r^6}\right)^{-1}, \quad \mu=1,\ldots ,3 \quad i=4,\ldots , 11,\end{align} }[/math]

where [math]\displaystyle{ \eta }[/math] is the flat-space metric and the distinction has been made between world volume [math]\displaystyle{ x^\mu }[/math] and transverse [math]\displaystyle{ x^i }[/math] coordinates. The constant [math]\displaystyle{ q }[/math] is proportional to the charge of the brane which is given by the integral of [math]\displaystyle{ F }[/math] over the boundary of the transverse space of the brane.^[2]

References

↑ K. Stelle, "BPS Branes in Supergravity"
↑ A. Miemiec, I. Schnakenburg "Basics of M-theory"

v t e String theory
Background	Strings History of string theory First superstring revolution Second superstring revolution String theory landscape
Theory	Nambu–Goto action Polyakov action Bosonic string theory Superstring theory Type I string Type II string Type IIA string Type IIB string Heterotic string N=2 superstring F-theory String field theory Matrix string theory Non-critical string theory Non-linear sigma model Tachyon condensation RNS formalism GS formalism
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Particles and fields	Graviton Dilaton Tachyon Ramond–Ramond field Kalb–Ramond field Magnetic monopole Dual graviton Dual photon
Branes	D-brane NS5-brane M2-brane M5-brane S-brane Black brane Black holes Black string Brane cosmology Quiver diagram Hanany–Witten transition
Conformal field theory	Virasoro algebra Mirror symmetry Conformal anomaly Conformal algebra Superconformal algebra Vertex operator algebra Loop algebra Kac–Moody algebra Wess–Zumino–Witten model
Gauge theory	Anomalies Instantons Chern–Simons form Bogomol'nyi–Prasad–Sommerfield bound Exceptional Lie groups (G₂, F₄, E₆, E₇, E₈) ADE classification Dirac string p-form electrodynamics
Geometry	Kaluza–Klein theory Compactification Why 10 dimensions? Kähler manifold Ricci-flat manifold Calabi–Yau manifold Hyperkähler manifold K3 surface G₂ manifold Spin(7)-manifold Generalized complex manifold Orbifold Conifold Orientifold Moduli space Hořava–Witten domain wall K-theory Twisted K-theory
Supersymmetry	Supergravity Superspace Lie superalgebra Lie supergroup
Holography	Holographic principle AdS/CFT correspondence
M-theory	Matrix theory Introduction to M-theory
String theorists	Aganagić Arkani-Hamed Atiyah Banks Berenstein Bousso Cleaver Curtright Dijkgraaf Distler Douglas Duff Ferrara Fischler Friedan Gates Gliozzi Gopakumar Green Greene Gross Gubser Gukov Guth Hanson Harvey Hořava Gibbons Kachru Kaku Kallosh Kaluza Kapustin Klebanov Knizhnik Kontsevich Klein Linde Maldacena Mandelstam Marolf Martinec Minwalla Moore Motl Mukhi Myers Nanopoulos Naqvi Năstase Nekrasov Neveu Nielsen van Nieuwenhuizen Novikov Olive Ooguri Ovrut Polchinski Polyakov Rajaraman Ramond Randall Randjbar-Daemi Roček Rohm Scherk Schwarz Seiberg Sen Shenker Siegel Silverstein Sơn Staudacher Steinhardt Strominger Sundrum Susskind 't Hooft Townsend Trivedi Turok Vafa Veneziano Verlinde Verlinde Wess Witten Yau Yoneya Zamolodchikov Zamolodchikov Zaslow Zumino Zwiebach

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M2-Brane

Description

See also

References