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F-theory and the Classification of LSTs
Tom Rudelius Harvard University
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Based On /hep-th with Jonathan Heckman, David Morrison*, and Cumrun Vafa /hep-th with Lakshya Bhardwaj, Michele Del Zotto, Jonathan Heckman, David Morrison*, and Cumrun Vafa *A very happy belated 60th birthday to Dave
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Recall from Jonathan Heckman’s Talk:
6D SCFTs have been classified via F-theory Nearly all F-theory conditions can be phrased in field theory terms 6D SCFTs = Generalized Quivers
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Recall from Jonathan Heckman’s Talk:
Looks like chemistry “Radicals” “Atoms”
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Classification Strategy
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Why study LSTs? LSTs serve as “toy model” for full string theory
LSTs sit between SCFTs and gravitational theories in 6D Understanding LSTs will help us understand these theories in more detail
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They are characterized by the presence of a non- dynamical tensor
Punchline #1 LSTs are UV complete, non-local 6D theories with gravity decoupled and an intrinsic string scale They are characterized by the presence of a non- dynamical tensor
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LSTs are “affinizations” of 6D SCFTs
Punchline #2 LSTs are “affinizations” of 6D SCFTs
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Punchline #3 Gauge algebras and matter content of 6D LSTs are tightly constrained by anomaly cancellation (similar to 6D SCFTs)
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Punchline #4 F-theory models of many LSTs feature a total space with two elliptic fibrations
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“Affinizing” SCFTs
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Example: (2,0) LSTs SCFTs LSTs
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A (1,0) Example SCFT LST
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Enhancing SCFT Fibers Enhancing LST Fibers 16 fundamentals, 2 antisym. tensors + 2 fundamentals adjoint hyper + 2 fundamentals 16 fundamentals, 2 antisym. tensors adjoint hyper
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adjoint hyper 16 fundamentals 1 antisym. tensor
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Conclusions LSTs are 6D theories with gravity decoupled, a non-dynamical tensor, and an intrinsic string scale The classification of 6D SCFTs enables the classification of LSTs via “affinization” Known T-dualities between LSTs are realized in F-theory as exchange of a double elliptic fibration
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Open Questions Non-geometric structures in F-theory?
Compactifications of LSTs? RG flows for LSTs? T-duality of general LSTs?
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