Abstract

We consider compactifications of rank \boldsymbol{Q}𝐐 E-string theory on a genus zero surface with no punctures but with flux for various subgroups of the \boldsymbol{\mathrm{E}_8\times \mathrm{SU}(2)}E8×SU(2) global symmetry group of the six dimensional theory. We first construct a simple Wess–Zumino model in four dimensions corresponding to the compactification on a sphere with one puncture and a particular value of flux, the cap model. Using this theory and theories corresponding to two punctured spheres with flux, one can obtain a large number of models corresponding to spheres with a variety of fluxes. These models exhibit interesting IR enhancements of global symmetry as well as duality properties. As an example we will show that constructing sphere models associated to specific fluxes related by an action of the Weyl group of \boldsymbol{\mathrm{E}_8}E8 leads to the S-confinement duality of the \boldsymbol{\mathrm{USp}(2Q)}USp(2𝐐) gauge theory with six fundamentals and a traceless antisymmetric field. Finally, we show that the theories we discuss possess an \boldsymbol{\mathrm{SU}(2)_{\text{ISO}}}SU(2)ISO symmetry in four dimensions that can be naturally identified with the isometry of the two-sphere. We give evidence in favor of this identification by computing the `t Hooft anomalies of the \boldsymbol{\mathrm{SU}(2)_{\text{ISO}}}SU(2)ISO in 4d and comparing them with the predicted anomalies from 6d.

Highlights

  • Introduction and SummaryIt is possible to construct a vast landscape of 4d Quantum Field Theories by considering a 6d CFT on a Riemann surface

  • We are going to construct the theory corresponding to the compactification of the rank Q E-string theory on a one punctured sphere with some value of flux for the E8 × SU(2)L global symmetry,4 which we shall call the cap model

  • For simplicity we only show the first few orders and the order pq containing the conserved currents, but we checked that the other terms organize into characters of the expected global symmetry

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Summary

Introduction and Summary

It is possible to construct a vast landscape of 4d Quantum Field Theories by considering a 6d CFT on a Riemann surface. This is a 6d (1, 0) SCFT obtained for example by considering Q M5 branes probing the “end-of-the-world” M9 brane in M-theory Compactifications of these models on two punctured spheres with particular value of flux and on tori were studied in [8,18]. In particular in Appendix C we discuss the SU(2)ISO global symmetry in 2 N = 1 A1 class S compactifications These are very simple 4d Lagrangian theories which exhibit the appearance of this geometric symmetry. It would be interesting to understand in what scenarios dualities with orthogonal groupsr and generalizations of the special unitary dualities with adjoint fields [26,27,28,29] make their appearance Another question is to understand the 3d reductions of the sphere theories and in particular whether they have mirror symmetry duals (See for example [30])

Derivation of the basic cap model
Examples of 2 models
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