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M-theory on 8-manifolds

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Contents

Idea

The KK-compactification of M-theory on fibers which are 8-manifolds. In the low-energy limiting 11-dimensional supergravity this is KK-compactification to 3d supergravity.

Typically this is considered with a reduction of the structure group on the compactification fiber from Spin(8) to Spin(7), in which case one speaks of M-theory on Spin(7)-manifolds (see the references below). Further reduction to G2-structure yields M-theory on G2-manifolds.

Properties

C-field tadpole cancellation condition

In M-theory compactified compact 8-manifold fibers, tadpole cancellation for the supergravity C-field (see also at C-field tadpole cancellation) is equivalently the condition

N M2+12(G 4[X (8)]) 2=148(p 212p 1 2)[X 8]I 8(X 8), N_{M2} \;+\; \tfrac{1}{2} \big( G_4[X^{(8)}]\big)^2 \;=\; \underset{ I_8(X^8) }{ \underbrace{ \tfrac{1}{48}\big( p_2 - \tfrac{1}{2}p_1^2 \big)[X^{8}] } } \;\;\;\; \in \mathbb{Z} \,,

where

  1. N M2N_{M2} is the net number of M2-branes in the spacetime (whose worldvolume appears as points in X (8)X^{(8)});

  2. G 4G_4 is the field strength/flux of the supergravity C-field

  3. p 1p_1 is the first Pontryagin class and p 2p_2 the second Pontryagin class combining to I8, all regarded here in rational homotopy theory.

If X 8X^{8} has

or

then

12(p 214(p 1) 2)=χ \tfrac{1}{2}\big( p_2 - \tfrac{1}{4}(p_1)^2 \big) \;=\; \chi

is the Euler class (see this Prop. and this Prop., respectively), hence in these cases the condition is equivalently

N M2+12(G 4[X (8)]) 2=124χ[X 8], N_{M2} \;+\; \tfrac{1}{2} \big( G_4[X^{(8)}]\big)^2 \;=\; \tfrac{1}{24}\chi[X^8] \;\;\;\; \in \mathbb{Z} \,,

where χ[X]\chi[X] is the Euler characteristic of XX.

For references see there.


Relation to F-theory

If the 8-dimensional fibers themselves are elliptic fibrations, then M-theory on these 8-manifolds is supposedly T-dual to F-theory KK-compactified to 3+13+1 spacetime-dimensions.

In particular, if there is an M2-brane filling the base 2+1-dimensional spacetime, this is supposedly T-dual to a 3+1-dimensional spacetime filling D3-brane in F-theory (e.g. Condeescu-Micu-Palti 14, p. 2)

For more on this see at F/M-theory on elliptically fibered Calabi-Yau 4-folds.


Black M2-branes and Exotic 7-spheres

The discovery of exotic 7-spheres proceeded via 8-manifolds XX with boundary homeomorphic to the 7-sphere X homeoS 7\partial X \simeq_{homeo} S^7, but not necessarily diffeomorphic to S 7S^7 with its canonical smooth structure (for more see there).

Hence when regarded from the point of view of M-theory on 8-manifolds, exotic 7-spheres arise as near horizon limits of peculiar black M2-brane spacetimes 2,1×X\mathbb{R}^{2,1} \times X.

See also Morrison-Plesser 99, section 3.2.

References

General

With Spin(7)Spin(7)-structure

Discussion of KK-compactification on 8-dimensional Spin(7)-manifolds (see also at M-theory on G2-manifolds):

With Sp(2)Sp(1)Sp(2)\cdot Sp(1)-structure

M-theory on HP^2, hence on a quaternion-Kähler manifold of dimension 8 with holonomy Sp(2).Sp(1), is considered in

and argued to be dual to M-theory on G2-manifolds in three different ways, which in turn is argued to lead to a a possible proof of confinement in the resulting 4d effective field theory (see there for more).

M2-brane spacetimes

Last revised on April 24, 2019 at 04:22:16. See the history of this page for a list of all contributions to it.