By reference to the superembedding formalism for super p-branes, the existence of “-branes” has been argued [Howe & Sezgin 1997, p. 8], for small natural numbers , with the following properties:
The -dimensional target spacetime carries flux densities
subject to the Bianchi identities
and on the brane’s worldvolume
there is a flux density
satisfying the Bianchi identity
In Howe, Raetzel & Sezgin 1998, p 3 this is claimed for . The followup article Howe, Raetzel & Rudychev 1999 considers it for .
For the above Bianchi identities read:
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 and ) of this form:
where in the last line is the chiral flux on the M5-brane worldvolume.
This makes the -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).
Original articles:
Paul S. Howe, Ergin Sezgin, p. 8 of: Superbranes, Phys. Lett. B 390 (1997) 133-142 [arXiv:hep-th/9607227, doi:10.1016/S0370-2693(96)01416-5]
Paul S. Howe, O. Raetzel, Ergin Sezgin, pp. 3-4 of: On Brane Actions and Superembeddings, JHEP 9808 (1998) 011 [arXiv:hep-th/9804051, doi:10.1088/1126-6708/1998/08/011]
Paul S. Howe, O. Raetzel, I. Rudychev, Ergin Sezgin: L-branes, Class. Quant. Grav. 16 (1999) 705-722 [arXiv:hep-th/9810081, doi:10.1088/0264-9381/16/3/006]
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.