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Massive IIA flux compactifications and U-dualities

T. Banks, K. van den Broek

TL;DR

This work analyzes the massive IIA flux compactifications of DeWolfe et al. by performing an approximate double T-duality to map to IIA on a twisted torus, then examining the backreaction of the orientifold and the resultant AdS$_4$ entropy scaling. The authors argue that in the single large-flux regime the entropy and backreaction point toward an M-theory interpretation with M2-branes, while in the all-flux regime 11D supergravity becomes unreliable and the geometry resembles a regionally varying, F-theory–like setup. They present a naive M-theory lift that is consistent only away from the orientifold locus, and they discuss how the Bianchi identities and supersymmetry conditions constrain the possible lifts, suggesting a weak $G_2$ holonomy seven-manifold near the M2-brane core. Overall, the paper contends that the DeWolfe et al. backgrounds likely do not admit a uniform weakly coupled 4D EFT description and that a more intricate, regionally valid framework—potentially a dual 2+1D CFT or F-theory–like structure—is needed to capture their quantum gravity dynamics.

Abstract

We attempt to find a rigorous formulation for the massive type IIA orientifold compactifications of string theory introduced in hep-th/0505160. An approximate double T-duality converts this background into IIA string theory on a twisted torus, but various arguments indicate that the back reaction of the orientifold on this geometry is large. In particular, an AdS calculation of the entropy suggests a scaling appropriate for N M2-branes, in a certain limit of the compactification, though not the one studied in hep-th/0505160. The M-theory lift of this specific regime is not 4 dimensional. We suggest that the generic limit of the background corresponds to a situation analogous to F-theory, where the string coupling is small in some regions of a compact geometry, and large in others, so that neither a long wavelength 11D SUGRA expansion, nor a world sheet expansion exists for these compactifications. We end with a speculation on the nature of the generic compactification.

Massive IIA flux compactifications and U-dualities

TL;DR

This work analyzes the massive IIA flux compactifications of DeWolfe et al. by performing an approximate double T-duality to map to IIA on a twisted torus, then examining the backreaction of the orientifold and the resultant AdS entropy scaling. The authors argue that in the single large-flux regime the entropy and backreaction point toward an M-theory interpretation with M2-branes, while in the all-flux regime 11D supergravity becomes unreliable and the geometry resembles a regionally varying, F-theory–like setup. They present a naive M-theory lift that is consistent only away from the orientifold locus, and they discuss how the Bianchi identities and supersymmetry conditions constrain the possible lifts, suggesting a weak holonomy seven-manifold near the M2-brane core. Overall, the paper contends that the DeWolfe et al. backgrounds likely do not admit a uniform weakly coupled 4D EFT description and that a more intricate, regionally valid framework—potentially a dual 2+1D CFT or F-theory–like structure—is needed to capture their quantum gravity dynamics.

Abstract

We attempt to find a rigorous formulation for the massive type IIA orientifold compactifications of string theory introduced in hep-th/0505160. An approximate double T-duality converts this background into IIA string theory on a twisted torus, but various arguments indicate that the back reaction of the orientifold on this geometry is large. In particular, an AdS calculation of the entropy suggests a scaling appropriate for N M2-branes, in a certain limit of the compactification, though not the one studied in hep-th/0505160. The M-theory lift of this specific regime is not 4 dimensional. We suggest that the generic limit of the background corresponds to a situation analogous to F-theory, where the string coupling is small in some regions of a compact geometry, and large in others, so that neither a long wavelength 11D SUGRA expansion, nor a world sheet expansion exists for these compactifications. We end with a speculation on the nature of the generic compactification.

Paper Structure

This paper contains 33 sections, 68 equations.