Math 2.0

Quantum theory Definition

Brane

Builds on Lorentzian manifoldSubmanifold

Definition

Let (M,g)(M, g) be a DD-dimensional Lorentzian manifold and let 0≤p≤D−10 \le p \le D - 1. A pp-brane in MM is an extended object whose history is a (p+1)(p+1)-dimensional submanifold W⊂MW \subset M, its worldvolume, on which the induced metric h=g∣Wh = g|_W is Lorentzian. In the simplest case its dynamics is given by the Nambu–Goto–Dirac action S[W]=−Tp∫W−det⁡hαβ  dp+1σ.S[W] = -T_p \int_W \sqrt{-\det h_{\alpha\beta}} \; d^{p+1}\sigma. Here σα\sigma^\alpha are coordinates on WW, hαβh_{\alpha\beta} are the components of hh, and Tp>0T_p > 0 is a constant, the tension of the brane.

Remarks

The action is −Tp-T_p times the (p+1)(p+1)-volume of WW, so the classical worldvolumes are those of stationary volume. Example: for p=0p = 0, WW is a timelike curve and SS is −T0-T_0 times its proper time. This is the action of a free relativistic particle of mass T0T_0, in units c=1c = 1. For p=1p = 1 one gets the Nambu–Goto action of a string. Non-example: a spacelike surface in MM is not the worldvolume of a brane, since its induced metric is not Lorentzian. A Dpp-brane in string theory is a pp-brane on which open strings can end, with Dirichlet boundary conditions in the normal directions. Its action, the Dirac–Born–Infeld action, also contains a gauge field on WW.

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  1. Lorentzian manifold concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Brane
About this page
TagWD5EM0V75H
URIm2://WD5EM0V75H
Kinddefinition
WritingW0 stub
MSC81T30, 83E30
DefinesBrane
UsesLorentzian manifold, Submanifold
Changed3 November 2026

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