Quantization of 10D Massless Superparticle by Lado Razmadze

Quantization of 10D Massless Superparticle by Lado Razmadze
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Delve into the fascinating world of quantizing gauge theories and relativistically invariant theories in curved spacetime through the study of 10D massless superparticles. Explore the algebraic approach using the Faddeev-Jackiw method, covariant quantization principles, and the use of Darboux's theorem. Understand the intricacies of canonical variables, Poisson brackets, and canonical commutator relations, all leading to the quantization of the 10D massless superparticle.

  • Gauge Theories
  • Relativistic Invariance
  • 10D Massless
  • Superparticles
  • Quantization

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  1. Quantization of 10d massless Quantization of 10d massless superparticle superparticle Lado Razmadze Supervisor: Prof. George Jorjadze Free University of Tbilisi 8 th Georgian German School and Workshop in Basic Science Tbilisi 23.08.2018

  2. Motivation Strings and Superstrings in AdS space Quantizing relativistically invariant theories in curved spacetime involve solving nonlinear Klein-Gordon equations Algebraic approach using Faddeev-Jackiw method is favorable. LR - Quantization of 10d massless superparticle

  3. Quantizing gauge theories LR - Quantization of 10d massless superparticle

  4. Quantizing gauge theories Covariant quantization first quantizes the gauge theory and then reduces the space of states by the condition ? corresponds to classical constraints. Hamiltonian reduction is done via gauge fixing or by choosing a complete set of gauge invariant variables. ? ?? = 0 where ? LR - Quantization of 10d massless superparticle

  5. Quantizing gauge theories Using Darboux s theorem we can always change to canonical variables ?????= ?? ?,? ????? Q and P are canonical coordinates of our reduced phase space LR - Quantization of 10d massless superparticle

  6. Quantizing gauge theories We can then rewrite our conserved quantities in terms of ?? and ?? Define canonical Poisson brackets as ??,??= 1 Use this to define canonical commutator relations After this we define Inner product so that the operators defined by the conserved quantities are self-adjoint LR - Quantization of 10d massless superparticle

  7. Brink-Schwartz action Consider superspace with coordinates ??,?? where ?? M10 and ?? are fermionic coordinates given by 32-component Majorana Majorana- -Weyl spinors Weyl spinors. ?? are Grassmann Grassmann numbers LR - Quantization of 10d massless superparticle

  8. Brink-Schwartz action 2 ?? ????? ? 2? ? = ?? ?<0 is associated with worldline metric ? = 0,1, ,9 ?0is defined as ?0= ? ?? matrices ? = 1, ,9 form Euclidean 9d Clifford Algebra Clifford Algebra ????+ ????= 2???? LR - Quantization of 10d massless superparticle

  9. Super-Algebra Our action is invariant under the transformations of the form ?? ??+ ??, ?? ??+? ? ? ? ? +? 2??????? +1 2?????, ? ? +1 2 ?? ??+ ?????, 2?0???? ??? 1 4??,??, ?,? = 1,2, ,9 LR - Quantization of 10d massless superparticle

  10. Super-Algebra Introducing the momentum variables ?? ????? ? ? ??= Corresponding charges are ??= ?? ??? ??= ?????? ???? ???= ???? ???? ????? ?0?= ??? ???0 1 ??? 2????? LR - Quantization of 10d massless superparticle

  11. Super-Algebra Introducing first order formalism ?? ????? ? +? 2?2 ? = ?? ?? ? plays a role of Lagrange multiplier and its variation ?2= 0 and defines energy of the particle ? = ?0 LR - Quantization of 10d massless superparticle

  12. Super-Algebra ?? ??, ??= ??? ? = 1,2, ,8 ?? are orthonormal solutions of ?? ??? ?= ??? ????? ? Factor of ? is added for convenience LR - Quantization of 10d massless superparticle

  13. Generator construction We take the presymplectic form ? = ????? ??????? We choose ??,?0?,??,?0,??as our variables ?0?+ ???0+1 ??? 2????? ??= ? ?0? ? ? ? = ??? 2?????? LR - Quantization of 10d massless superparticle

  14. Generator construction Using the solutions of ?? ? = ?????+? 2????? ? ??=?0? ? ???? ??? ??????, ??= ?? 2?? ?? ? ?????? We neglected d ???? LR - Quantization of 10d massless superparticle

  15. Generator construction We use first 8x8 block of ??matrices ?= 0, 9 ??? 1 ? < 8, ??? = ??? 8 orthonormal vectors can be chosen as 1 ?? = ? ?? ????+ ????? 2? ? + ?9 ? = 1,2, ,8 , ? = 1,2, ,16 LR - Quantization of 10d massless superparticle

  16. Generator construction ?? Using the defined vectors we write out ?? ??=?????? ???? 4? ? + ?9 ?? ?? Now we rewrite rotation generator using invariant variables ???= ???? ????+? 1 2??????? ???? ???? ????? ?? ???? ??????+ ???? 2 ???? LR - Quantization of 10d massless superparticle

  17. Thank you! Thanks to VW-Stiftung for the opportunity of continuing my studies in Bonn I intend to continue working on superstings in AdS LR - Quantization of 10d massless superparticle

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