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On HS symmetries, cubic interactions, AdS & CFT Massimo Taronna - PowerPoint PPT Presentation

On HS symmetries, cubic interactions, AdS & CFT Massimo Taronna Albert Einstein Institute (Berlin-Potsdam-Golm) based on arXiv:1311.0242 w. E.Joung and arXiv:1305.5180 w. N.Boulanger, D.Ponomarev, E.Skvortsov 1 Desired Goals! Uncover


  1. On HS symmetries, cubic interactions, AdS & CFT Massimo Taronna Albert Einstein Institute (Berlin-Potsdam-Golm) based on arXiv:1311.0242 w. E.Joung and arXiv:1305.5180 w. N.Boulanger, D.Ponomarev, E.Skvortsov 1

  2. Desired Goals! • Uncover the symmetries behind String Theory • Shed light on holography and Quantum Gravity 2

  3. 3

  4. ...topology matters!! 4

  5. History teaches us: Symmetry has always paid off! HS Gravity! Symmetry What is the “maximal” symmetry of Quantum Gravity? Fradkin & Vasiliev (‘80s): Higher-Spin Symmetry! 3

  6. Cons: too big symmetry => too simple theory... Pros: • Deformation (gauging) of symmetries (Algebroid, field dependent structure constants) • Almost all checks of AdS/CFT driven by symmetry (maximal symmetry => proof of Holography?) 4

  7. To do List • HS systematics Some of this today • HS holography • HS on non-trivial backgrounds (black-holes!) • … 5

  8. Cubic Couplings Classification E.Joung and M.T. ‘13 6

  9. Coleman-Mandula in AdS/CFT! Assumptions: symmetric tensors + one HS generator + no colour (+ Gravity)! Boulanger, Ponomarev, Skvortsov , M.T. ‘13 UIR Algebra: AdS 3 /CFT 2 (Virasoro!!) Scalar & Spinor Moyal (unique) AdS 4 /CFT 3 Singletons Fradkin, Vasiliev ‘86; Konstein, Vasiliev ‘90; Maldacena, Zhiboedov 2011 One parameter family AdS 5 /CFT 4 (doubletons) Gunaydin et all; Boulanger, Skvortsov; Manvelyan, Mkrtcyan, Mkrtcyan, Theisen AdS 6+n /CFT 5+n Scalar singleton 7

  10. Outlook • Admissibility will put further constraints • Deformation (Lie Algebroids!) • More general backgrounds (Black-Holes!) 8

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