Abstract

Abstract We analyze the basic M2-M5 intersection in the supergravity regime using the blackfold approach. This approach allows us to recover the 1/4-BPS self-dual string soliton solution of Howe, Lambert and West as a three-funnel solution of an effective fivebrane worldvolume theory in a new regime, the regime of a large number of M2 and M5 branes. In addition, it allows us to discuss finite temperature effects for non-extremal self-dual string soliton solutions and wormhole solutions interpolating between stacks of M5 and anti-M5 branes. The purpose of this paper is to exhibit these solutions and their basic properties.

Highlights

  • (2) As a three-funnel solution of the Basu-Harvey equation [3], which has been proposed as an M-theoretic generalization of the Nahm equations for the BIon

  • It allows us to discuss finite temperature effects for non-extremal self-dual string soliton solutions and wormhole solutions interpolating between stacks of M5 and anti-M5 branes

  • In the present case we will be interested in the effective fivebrane worldvolume dynamics of the M2-M5 bound state [13,14,15,16,17]

Read more

Summary

Planar M2-M5 bound state

Our starting point is a well-known exact solution of the eleven dimensional supergravity equations of motion that describes the black M2-M5 bound state [13,14,15,16,17]. The solution, which describes M2 brane charge dissolved into the worldvolume of the black fivebrane along the (012) plane, is parameterized by the constants r0, α and θ which control the temperature, the M2 and the M5 brane charge. Ε denotes the energy density, T the temperature, s the entropy density, Q5 the fivebrane charge, Q2 the twobrane charge density, and Φ5, Φ2 the corresponding chemical potentials. We will reserve the notation Q for charges and Q for charge densities. Where, following closely the notation of [10], ua denotes a unit 6-velocity field, ηab the flat induced worldvolume metric, and h(aqb) (q = 2, 5) is a projector along the worldvolume directions of the M2 and M5 branes respectively.

Leading order blackfold equations
Static ansatz
Q2 4π2 Q5
Thermal spikes
Extremal wormholes
Branch connected to extremal wormholes
Wormholes of the neutral branch
Summary and further work

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.