Abstract

AdS7 solutions of massive type IIA have been classified, and are dual to a large class of six-dimensional (1, 0) SCFT’s whose tensor branch deformations are described by linear quivers of SU groups. Quivers and AdS vacua depend solely on the group theory data of the NS5-D6-D8 brane configurations engineering the field theories. This has allowed for a direct holographic match of their a conformal anomaly. In this paper we extend the match to cases where O6 and O8-planes are present, thereby introducing SO and USp groups in the quivers. In all of them we show that the a anomaly computed in supergravity agrees with the holographic limit of the exact field theory result, which we extract from the anomaly polynomial. As a byproduct we construct special AdS7 vacua dual to nonperturbative F-theory configurations. Finally, we propose a holographic a-theorem for six-dimensional Higgs branch RG flows.

Highlights

  • Six-dimensional superconformal field theories (SCFT’s ) have received a great deal of attention in recent years

  • In all of them we show that the a anomaly computed in supergravity agrees with the holographic limit of the exact field theory result, which we extract from the anomaly polynomial

  • We provide further compelling evidence for the advocated duality between the AdS7 vacua of [27, 30], the brane configurations of [3, 4], and a vast class of (1, 0) SCFT’s. To obtain such a result we had to generalize the simple combinatorial formalism of [1] in order to construct more general AdS7 vacua featuring orientifold sources. (The possiblity of having vacua with an O8-plane source was suggested in [30] but left unexplored. [52] recently constructed a first concrete example which is dual to the so-called massive E-string theory.) As an interesting byproduct of this, we exhibit for the first time the supergravity duals to some of the “formal” massive IIA brane setups of [32], which are characterized by the same a conformal anomaly as certain nonperturbative F-theory configurations

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Summary

Introduction

Six-dimensional superconformal field theories (SCFT’s ) have received a great deal of attention in recent years. There it was shown that the a conformal anomaly of (1, 0) theories engineered by NS5-D6-D8 brane configurations in type IIA perfectly agrees with the supergravity result computed using the massive AdS7 vacua of [27, 30] Emboldened by this nontrivial result, we extend the six-dimensional holographic a anomaly match to cases where orientifolds are present.. [52] recently constructed a first concrete example which is dual to the so-called massive E-string theory.) As an interesting byproduct of this, we exhibit for the first time the supergravity duals to some of the “formal” massive IIA brane setups of [32], which are characterized by the same a conformal anomaly as certain nonperturbative F-theory configurations We argue that these type IIA AdS7 solutions can be understood as gravity duals to the Ftheory quivers, complementing a very scarce class of AdS vacua of type IIB with varying and monodromic axiodilaton.

Only SU(k) groups: M5’s on C2/Zk
Alternating SO-USp groups
SO or USp flavor, USp, SO, SU gauge groups: O8± onto D8’s
The holographic limit
Constructing generic solutions with z
Boundary conditions
Computation of a in field theory
SU quivers on the tensor branch
Alternating SO-USp quivers on the tensor branch
Quivers from brane configurations with an O8-plane
Computation of a in O8+ and D8-O8− theories
Quivers from brane configurations with O6-planes and an O8-plane
Holographic match
Solutions with regular or D6 poles
Solutions with O6-planes
Solutions with an O8 at z = 0, regular or D6 pole at z = N
Solutions with an O8 at z = 0, and O6-planes
New examples
A formal massive IIA quiver and its dual vacuum
The gravity dual of the O8− with O6-planes
On the holographic a-theorem
Conclusions
A Change of variables: from y to z
B Integration constants and boundary data
Recovering [1, appendix A]: only regular poles
Symmetric case
Asymmetric case
Generic poles: none among r0, rN , α0, αN is zero
We perform the sums
Full Text
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