Abstract:We compare the sets of Calabi-Yau threefolds with large Hodge numbers that are constructed using toric hypersurface methods with those can be constructed as elliptic fibrations using Weierstrass model techniques motivated by F-theory. There is a close correspondence between the structure of "tops" in the toric polytope construction and Tate form tunings of Weierstrass models for elliptic fibrations. We find that all of the Hodge number pairs (h 1,1 , h 2,1 ) with h 1,1 or h 2,1 ≥ 240 that are associated with t… Show more
“…Examples are the conformal matter theories [45], which have a particularly nice characterization in terms of non-flat resolutions of the (noncompact) elliptically fibered Calabi-Yau threefold. In the context of F-theory, such fibrations have been systematically studied in [46] for Kodaira fibers, with examples in codimension two and three appearing in [13,29,[47][48][49][50][51][52][53][54][55][56][57]. Unlike the more commonly studied resolutions of minimal collisions of elliptic singularities [58][59][60][61][62], which result in complex one-dimensional fibers, non-minimal singularities require insertions of complex surfaces, S i , into the fiber in order to resolve the singularity.…”
Section: Part Ii: Box Graphs and Coulomb Branch Phasesmentioning
We propose a graph-based approach to 5d superconformal field theories (SCFTs) based on their realization as M-theory compactifications on singular elliptic Calabi-Yau threefolds. Fieldtheoretically, these 5d SCFTs descend from 6d N = (1, 0) SCFTs by circle compactification and mass deformations. We derive a description of these theories in terms of graphs, so-called Combined Fiber Diagrams, which encode salient features of the partially resolved Calabi-Yau geometry, and provides a combinatorial way of characterizing all 5d SCFTs that descend from a given 6d theory. Remarkably, these graphs manifestly capture strongly coupled data of the 5d SCFTs, such as the superconformal flavor symmetry, BPS states, and mass deformations.The capabilities of this approach are demonstrated by deriving all rank one and rank two 5d SCFTs. The full potential, however, becomes apparent when applied to theories with higher rank. Starting with the higher rank conformal matter theories in 6d, we are led to the discovery of previously unknown flavor symmetry enhancements and new 5d SCFTs.
“…Examples are the conformal matter theories [45], which have a particularly nice characterization in terms of non-flat resolutions of the (noncompact) elliptically fibered Calabi-Yau threefold. In the context of F-theory, such fibrations have been systematically studied in [46] for Kodaira fibers, with examples in codimension two and three appearing in [13,29,[47][48][49][50][51][52][53][54][55][56][57]. Unlike the more commonly studied resolutions of minimal collisions of elliptic singularities [58][59][60][61][62], which result in complex one-dimensional fibers, non-minimal singularities require insertions of complex surfaces, S i , into the fiber in order to resolve the singularity.…”
Section: Part Ii: Box Graphs and Coulomb Branch Phasesmentioning
We propose a graph-based approach to 5d superconformal field theories (SCFTs) based on their realization as M-theory compactifications on singular elliptic Calabi-Yau threefolds. Fieldtheoretically, these 5d SCFTs descend from 6d N = (1, 0) SCFTs by circle compactification and mass deformations. We derive a description of these theories in terms of graphs, so-called Combined Fiber Diagrams, which encode salient features of the partially resolved Calabi-Yau geometry, and provides a combinatorial way of characterizing all 5d SCFTs that descend from a given 6d theory. Remarkably, these graphs manifestly capture strongly coupled data of the 5d SCFTs, such as the superconformal flavor symmetry, BPS states, and mass deformations.The capabilities of this approach are demonstrated by deriving all rank one and rank two 5d SCFTs. The full potential, however, becomes apparent when applied to theories with higher rank. Starting with the higher rank conformal matter theories in 6d, we are led to the discovery of previously unknown flavor symmetry enhancements and new 5d SCFTs.
“…This rank-preserving tuning between SU (2) and G2 connects two phases of the same Calabi-Yau geometry. 11 Additional vertices from tops for all generic fibrations over Hirzebruch surfaces can be looked up in Table 11 in [15].…”
We find that for many Calabi-Yau threefolds with elliptic or genus one fibrations mirror symmetry factorizes between the fiber and the base of the fibration. In the simplest examples, the generic CY elliptic fibration over any toric base surface B that supports an elliptic Calabi-Yau threefold has a mirror that is an elliptic fibration over a dual toric base surfaceB that is related through toric geometry to the line bundle −6K B . The Kreuzer-Skarke database includes all these examples and gives a wide range of other more complicated constructions where mirror symmetry also factorizes. Since recent evidence suggests that most Calabi-Yau threefolds are elliptic or genus one fibered, this points to a new way of understanding mirror symmetry that may apply to a large fraction of smooth Calabi-Yau threefolds. The factorization structure identified here can also apply for Calabi-Yau manifolds of higher dimension.A The 16 reflexive 2D fiber polytopes ∇ 2 26 B Faces of the base polytope and chains of non-Higgsable clusters 26 the G2 has one additional fundamental (7), which contributes another 6 hypermultiplets charged under the Cartan, canceling the difference in dimension between SU (2) and G2. This rank-preserving tuning between SU (2) and G2 connects two phases of the same Calabi-Yau geometry. 11 Additional vertices from tops for all generic fibrations over Hirzebruch surfaces can be looked up in Table 11 in [15].
“…The problem of identifying 2D subpolytopes from the combinatorial data of a 4D polytope is described and discussed in some detail in [26,27,23]. We use here the notation and conventions of [22,23], to which the reader is referred for further background and references.…”
Section: Reflexive Subpolytopes and Fibrationsmentioning
confidence: 99%
“…A condition stated in [25] is that the base B of such a fibration should be identified by constructing the 2D toric variety from the set of primitive rays in the image of ∇ under the projection that takes ∇ 2 → 0. Indeed, in many cases, such as the "standard stacking" polytopes corresponding to many generic and (Tate) tuned Weierstrass models over a given base, one can use the structure of the polytopes and tops to determine the base and additional tuned Kodaira singularity types to directly construct a Weierstrass model for an elliptic fibration over the given base, thus identifying a Calabi-Yau threefold that is elliptically fibered and has the requisite Hodge numbers associated with the polytope, circumventing the explicit construction of fans compatible with a toric morphism from ∇ to ∇ 2 [22]. Particularly for more complicated fibrations with general fibers and twists, however, there is no systematic methodology for implementing such a direct construction; and in any case, it is desirable to know in general which triangulations of ∇ are compatible with the fibration structure, and whether in fact such triangulations always exist.…”
Section: Fibrations Of Polytopes Versus Toric Varietiesmentioning
confidence: 99%
“…It was shown in [20] that many polytopes in the Kreuzer-Skarke (KS) database [21] have a structure compatible with a K3 fibration. A systematic construction of elliptic CY threefolds at large Hodge numbers over toric base surfaces [22] showed that all Hodge number pairs in the KS database with h 1,1 ≥ 240 or h 2,1 ≥ 240 are associated with such elliptic Calabi-Yau threefolds. A systematic direct study of the fibration structure of the polytopes in the KS database was initiated in [23]; in that paper we found that all polytopes associated with Calabi-Yau threefolds having h 1,1 ≥ 150 or h 2,1 ≥ 150 have a reflexive 2D subpolytope, indicating a structure compatible with the presence of an elliptic or genus one fibration for the associated CY threefolds.…”
We find through a systematic analysis that all but 29,223 of the 473.8 million 4D reflexive polytopes found by Kreuzer and Skarke have a 2D reflexive subpolytope. Such a subpolytope is generally associated with the presence of an elliptic or genus one fibration in the corresponding birational equivalence class of Calabi-Yau threefolds. This extends the growing body of evidence that most Calabi-Yau threefolds have an elliptically fibered phase. arXiv:1907.09482v2 [hep-th]
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