Abstract

We argue for the quantum-gravitational inconsistency of certain 6d $\mathcal{N}=(1,0)$ supergravity theories, whose anomaly-free gauge algebra $\mathfrak{g}$ and hypermultiplet spectrum $M$ were observed in arxiv:2012.01437 to be realizable only as part of a larger gauge sector $(\mathfrak{g}' \supset \mathfrak{g}, M' \supset M)$ in F-theory. To detach any reference to a string theoretic method of construction, we utilize flavor symmetries to provide compelling reasons why the vast majority of such $(\mathfrak{g},M)$ theories are not compatible with quantum gravity constraints, and how the "automatic enhancement" to $(\mathfrak{g}', M')$ remedies this. In the first class of models, with $\mathfrak{g}' = \mathfrak{g} \oplus \mathfrak{h}$, we show that there exists an unbroken flavor symmetry $\mathfrak{h}$ acting on the matter $M$, which, if ungauged, would violate the No-Global-Symmetries Hypothesis. This argument also applies to 1-form center symmetries, which govern the gauge group topology and massive states in representations different than those of massless states. In a second class, we find that $\mathfrak{g}$ is incompatible with the flavor symmetry of certain BPS strings that must exist by the Completeness Hypothesis.

Highlights

  • AND SUMMARYPhysical features of string compactifications are highly constrained by geometric restrictions on the underlying compactification space

  • In the first class of models, with g0 1⁄4 g ⊕ h, we show that there exists an unbroken flavor symmetry h acting on the matter M, which, if ungauged, would violate the no-global-symmetries hypothesis

  • We find that g is incompatible with the flavor symmetry of certain supersymmetric strings that must exist by the completeness hypothesis

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Summary

INTRODUCTION

Physical features of string compactifications are highly constrained by geometric restrictions on the underlying compactification space. II E, we further comment on the relationship of the aforementioned obstructions to the validity of the “massless charge sufficiency conjecture” [39] in 6D supergravity theories While these arguments provide a consistent interpretation of the automatic enhancement conjecture in the larger web of quantum gravity constraints, this bottom-up perspective does not provide the means to rule out UVbreaking mechanisms not captured by anomalies; the observed enhancement is only a post factum confirmation of the absence of such a breaking. From the world sheet perspective, it is the spacetime symmetry g that plays the role of a global, or flavor, symmetry In this case, the specific type of strings (with charge b) present in the supergravity theory can constrain the symmetry algebra g, even if it is consistent with gauge anomalies in the 6D bulk. IV, we discuss some open questions about the automatic enhancement conjecture that needs further study of BPS strings of 6D supergravity theories to elucidate

AUTOMATIC ENHANCEMENT AS GAUGING OF FLAVOR SYMMETRIES
Review of 6D gauge anomalies
Cancellation of flavor anomalies
Examples
Other cases
Gauge group topology from gauged 1-form symmetries
Comment on the massless charge sufficiency conjecture
AUTOMATIC ENHANCEMENT ENFORCED BY BPS STRINGS
Automatic enhancement enforced by the E-string
Automatic enhancement enforced by the M-string
DISCUSSION
Full Text
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