Abstract
We present a prescription in F-theory for realizing matter in “exotic” representations of product gauge groups. For 6D vacua, bifundamental hypermultiplets are engineered by starting at a singular point in moduli space which includes 6D superconformal field theories coupled to gravity. A deformation in Higgs branch moduli space takes us to a weakly coupled gauge theory description. In the corresponding elliptically fibered Calabi-Yau threefold, the minimal Weierstrass model parameters (f, g, Δ) vanish at collisions of the discriminant at least to order (4, 6, 12), but with sufficiently high order of tangency to ensure the existence of T-brane deformations to a weakly coupled gauge theory with exotic bifundamentals. We present explicit examples including bifundamental hypermultiplets of {mathfrak{e}}_7times mathfrak{s}{mathfrak{u}}_2 and {mathfrak{e}}_6times mathfrak{s}{mathfrak{u}}_3 , each of which have dual heterotic orbifold descriptions. Geometrically, these matter fields are delocalized across multiple points of an F-theory geometry. Symmetry breaking with such representations can be used to produce high dimension representations of simple gauge groups such as the four-index symmetric representation of mathfrak{s}{mathfrak{u}}_2 and the three-index symmetric representation of mathfrak{s}{mathfrak{u}}_3 , and after further higgsing can yield discrete non-abelian symmetries.
Highlights
Perturbative open string theories involve matter in various two-index representations of the classical gauge groups U(N ), SO(N ), Sp(N )
We present a prescription in F-theory for realizing matter in “exotic” representations of product gauge groups
The appearance of matter in high dimension representations of continuous gauge groups and non-abelian discrete gauge groups are related since the latter can be obtained by giving vevs to scalars transforming in high dimension representations [21]
Summary
We present a general prescription for constructing examples in F-theory of matter in “exotic” bifundamental representations. In heterotic terms we can dissolve these instantons as flux inside the E8 locus, leading to a weakly coupled point of moduli space In these cases as well, T-brane deformations are available which leave the Weierstrass model unchanged. Taking into account these considerations, we see that even when we encounter collisions of the discriminant locus which do not remain in Kodaira-Tate form, the physical theory may be described by a weakly coupled model From this perspective, to engineer examples of “exotic” bifundamental representations, we apply the following procedure:. By tuning to a singular point in moduli space, we reach a theory coupled to 6D SCFTs, as well as its Higgs branch and tensor branch deformations This setting is dual to heterotic compactification on a K3 with 24 mobile instantons, of which the T 4/Z2 orbifold is a special limit [52]
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