nLab L-brane

Redirected from "Chern root".
Note: Chern class and splitting principle both redirect for "Chern root".

Context

Quantum field theory

String theory

Contents

Idea

By reference to the superembedding formalism for super p-branes, the existence of “L pL_p-branes” has been argued [Howe & Sezgin 1997, p. 8], for small natural numbers pp, with the following properties:

The p+4p+4-dimensional target spacetime X p+4X^{p+4} carries flux densities

G 2 Ω dR 2(X p+4) G p+1 Ω dR p+1(X p+4) G p+2 Ω dR p+2(X p+4), \begin{aligned} G_2 & \in \Omega^2_{dR}\big(X^{p+4}\big) \\ G_{p+1} & \in \Omega^{p+1}_{dR}\big(X^{p+4}\big) \\ G_{p+2} & \in \Omega^{p+2}_{dR}\big(X^{p+4}\big) \mathrlap{\,,} \end{aligned}

subject to the Bianchi identities

dG 2 =0 dG p+1 =0 dG p+2 =G 2G p+1; \begin{aligned} \mathrm{d} G_2 & = 0 \\ \mathrm{d} G_{p+1} & = 0 \\ \mathrm{d} G_{p+2} & = G_2 \wedge G_{p+1} \mathrlap{\,;} \end{aligned}

and on the brane’s worldvolume

Σ p+1ϕX p+4 \Sigma^{p+1} \xrightarrow{\phantom{-}\phi\phantom{-}} X^{p+4}

there is a flux density

F p Ω dR p(X p+1) \begin{aligned} F_p & \in \Omega^p_{dR}(X^{p+1}) \end{aligned}

satisfying the Bianchi identity

dF p =ϕ *G p+1. \begin{aligned} \mathrm{d} \, F_p & = \phi^\ast G_{p+1} \,. \end{aligned}

In Howe, Raetzel & Sezgin 1998, p 3 this is claimed for p{1,2,3,4,5}p \in \{1,2,3,4,5\}. The followup article Howe, Raetzel & Rudychev 1999 considers it for p{3,4,5}p \in \{3,4,5\}.

Examples

L 1L_1-brane

For p=1p = 1 the above Bianchi identities read:

dG 2 =0 dG 3 =G 2G 2 dH 1 =ϕ *G 2. \begin{aligned} \mathrm{d} G_2 & = 0 \\ \mathrm{d} G_3 & = G_2 \wedge G_2 \\ \mathrm{d} H_1 & = \phi^\ast G_2 \mathrlap{\,.} \end{aligned}

The first two are the Bianchi identities of 5D Maxwell-Chern-Simons theory, hence of the gauge sector of minimal D=5 supergravity.

There is a close structural analogy between this D=5 supergravity on one hand and D=11 supergravity on the other. The latter has Bianchi identities (for the supergravity C-field flux densities G 4G_4 and G 7G_7) of this form:

dG 4 =0 dG 7 =G 4G 4 dH 3 =ϕ *G 4, \begin{aligned} \mathrm{d} G_4 & = 0 \\ \mathrm{d} G_7 & = G_4 \wedge G_4 \\ \mathrm{d} H_3 & = \phi^\ast G_4 \mathrlap{\,,} \end{aligned}

where in the last line H 3H_3 is the chiral flux on the M5-brane worldvolume.

This makes the L 1L_1-brane structure above look like it matches the probe brane version of the known black string of D=5 supergravity (for which cf. Mizoguchi & Ohta 1998, Fujii, Kemmoku & Mizoguchi 2000).

References

Original articles:

Review:

Last revised on October 8, 2025 at 07:52:58. See the history of this page for a list of all contributions to it.