We consider a novel class of Weyl-conformally invariant p-brane theories which describe intrinsically light-like branes for any odd world-volume dimension, hence the acronym WILL-branes (Weyl-Invariant Light-Like branes). We discuss in some detail the prop
ν √
(56)
(brane)Tµν
FortheWILL-membranesubsystemwecanuseinsteadoftheaction(53)itsdualone(similartothesimplercaseEq.(8)versusEq.(23)):
dualSWILL brane= FρκFσλGρσGκλ,4 (4) x X(σ)δ3Φ( )γab aXκ bXλ,≡ GµκGνλdσ G µ3(4)x X(σ)εabcFbc aXµ.j≡qdσδ(57)(58)1 γγab( aX bX),
isgivenby:(59)wherethevariablebranetensionχ≡
χ(γ,u,A)≡ Φ( ) γ
2χ(γ,u,A)√
2γcd( cX dX) ( au qAa)( bu qAb)
γγab( bu qAb)
√ γγab bXµ+χ(γ,u,A)
r,forr<r0≡rhorizon=2GM1.(66)
Reissner-Norstr¨omblackholeoutsidethehorizon:
A(r)≡A+(r)=1 2GM2
r2,forr>r0≡rhorizon,(67)
44whereQ2=8πq2rhorizon≡128πq2G4M1;
FortheMaxwellsubsystemwehaveA1=...=AD 1=0everywhereand:
8