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added the statement of I8 appearing as the O(ℓ6) higher curvature correction to 11d supergravity (here):
A systematic analysis of the possible supersymmetric higher curvature corrections of D=11 supergravity makes the I8 appear as the higher curvature correction at order ℓ6, where ℓ is the Planck length in 11d (Souères-Tsimpis 17, Section 4).
At this order, the equation of motion for the supergravity C-field flux G4 and its dual G7 is (Souères-Tsimpis 17, (4.3))
dG7(ℓ)=−12G4(ℓ)∧G4(ℓ)+ℓ6I8,where the flux forms themselves appear in their higher order corrected form as power series in the Planck length
G4(ℓ)=G4+ℓ6G(1)4+⋯Yeah, but it’s more complicated:
They write tr(R2) instead of p1. The conversion factor for thee two should be 1/4π2, but of course it depends on conventions. Worse, when deriving the ℓ6-correction, they ignore the ℓ3-correction but then “absorb a numerical factor” in ℓ6 (below (4.3)). So at this point the two ℓ-s in the two prefactors are not even the same anymore.
So what I did in the entry was that I took for the ℓ3-term the prefactor that I know from other reasons to be there. Then the ℓ6 term is correct for some rescaling of ℓ. Of course there should really be a comment on that step in the entry.
And it would be good to sort out the actual relative factor between these two correction terms. If you are interested in digging into this, please let me know.
Sure, I’d be interested to have a look. Teaching is over, so have a bit more time now.
added pointer to:
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