nLab
cubical structure in M-theory

Contents

Context

String theory

Cohomology

cohomology

Special and general types

Special notions

Variants

Extra structure

Operations

Theorems

Contents

Idea

It is well known that when the higher Chern-Simons term in 11-dimensional supergravity is compactified on a 4-sphere to yield the 7-dimensional Chern-Simons theory which inside AdS7/CFT6 is dual to the M5-brane 6d (2,0)-superconformal QFT, the cup product square in ordinary differential cohomology that enters its definition is to receive a quadratic refinement. This was originally argued in (Witten 97) and then formalized and proven in (Hopkins-Singer 02).

What though is the situation up in 11 dimensions before compactifying to 7-dimensions?

In (DFM 03, section 9) it is claimed that the full 11-dimensional Chern-Simons term evaluated on the supergravity C-field (with its flux quantization correction, see there) indeed carries a cubic refinement.

More precisely, and slightly paraphrasing, the transgression XCS 11(C^)\int_X CS_{11}(\hat C) of the 11-dimensional Chern-Simons term of 11d SuGra to 10d spacetime XX is a complex line bundle on the moduli space CField(X)CField(X) of supergravity C-fields C^\hat C is claimed to be such that its “cubical line” Θ( XCS 11(C^))\Theta(\int_X CS_{11}(\hat C)) (in the notation at cubical structure on a line bundle) is the line bundle on the space of triples of C-field configurations which is given by the transgression of the three-fold cup product in ordinary differential cohomology,

Θ( XCS 11()) X() 1() 2() 3. \Theta\left(\int_X CS_{11}\left(-\right)\right) \simeq \int_X (-)_1 \cup (-)_2 \cup (-)_3 \,.

Relation to F-theory and the topological Witten genus

In the context of “F-theory compactifications” of M-theory, one considers C-fields on an elliptic fibration which are “factorizable fluxes”, in that their underlying cocycle C^\hat C in ordinary differential cohomology is the cup product of a cocycle C^ fib\hat C_{fib} on the fiber with one C^ b\hat C_b on the base

C^C^ bC^ fib. \hat C \coloneqq \hat C_{b} \cup \hat C_{fib} \,.

In approaches like (GKP 12 (around p. 19), KMW 12) the C-field is factored as a cup product of a degree-2 cocycle on the elliptic fiber with a degree-2 class in the Calabi-Yau-base. This makes the component of the C-field on the elliptic fiber a complex line bundle (with connection). Notice that the space of complex line bundles on an elliptic curve is dual to the elliptic curve itself.

On the other hand in e.g. (DFM 03, p.38) the factorization is taken to be that of two degree-3 cocycles in the base (which are then identified with the combined degree-3 RR-field/B-field flux coupled to the (p,q)-string) with, respectively, the two canonical degree-1 cocycles t^ i\hat t_i on the elliptic fiber which are given by the two canonical coordinate functions t it_i (speaking of a framed elliptic curve). In this case the fiber-component of the supergravity C-field “is” the elliptic curve-fiber,

C^B^ NSt^ 1+B^ RRt^ 2 \hat C \coloneqq \hat B_{NS} \cup \hat t_1 + \hat B_{RR} \cup \hat t_2

or equivalently each point in the moduli space of HH-flux in 10d induces an identification of the GG-flux with the elliptic curve this way.

This is maybe noteworthy in that when the C-field is identified with the compactification elliptic curve in this way, then the formula for Θ( XCS 11(C^))\Theta\left(\int_X CS_{11}(\hat C)\right) as above is exactly that appearing in the definition of a cubical structure on a line bundle over an elliptic curve. But a “cubical” trivialization of Θ(𝒪({0}))\Theta(\mathcal{O}(-\{0\})) over a given elliptic curve is what in (Hopkins 02, AHS01) is used to induce the sigma-orientation of the corresponding elliptic cohomology theory and in totality the string-orientation of tmf. But that is the refinement of the Witten genus, hence of the partition function of the heterotic string.

Now,by the above fact that Θ(CS 11()) X() 1() 2() 3\Theta\left(CS_{11}(-)\right) \simeq \int_X (-)_1 \cup (-)_2 \cup (-)_3 a cubical trivialization of Θ(L)\Theta(L) is also given by a trivialization of the topological class of the C-field. This is one way (or is at least closely related) to the trivialization of the anomaly line bundle which “sets the quantum integrand” of M-theory.

So there is a curious coincidence of concepts here, which might want to become a precise identification:

on the one hand there is naturally a cubical structure on a line bundle on the Chern-Simons line bundle over the moduli space of supergravity C-fields which for F-theory compactifications and factorizable flux configurations induces in particular a cubical structure on a line bundle over the compactification elliptic curve. On the other hand, the latter are the structures that enter the refined construction of the Witten genus via the string orientation of tmf.

Relation to S-duality and 3-form flux

The refined perspective on perturbative type II string theory is that (see also at orientifold) the B-field is a cocycle in (twisted) ordinary differential cohomology, while the RR-field is a cocycle in differential K-theory (im fact KR-theory). This is however not compatible with non-perturbative S-duality, which mixes the degree- components here.

In (DFM 03, section 9.3) it was argued that the cubical structure on the 11d CS term alleviates this problem, even though at face value it does not really solve it. But see at S-duality – Cohomological nature of type II fields for more on this.

Last revised on April 24, 2019 at 02:16:08. See the history of this page for a list of all contributions to it.