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Covariant quantization of the Superstring with fundamental b-c ghosts. Kiyoung Lee (Stony Brook) 2006. 5. 4. UNC
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Outline 1. Brief History 2. Review of 1 st quantized BRST formalism 3. Superparticle BRST 4. Superparticle BRST in SYM background 5. Superstring BRST 6. Amplitudes 7. Conclusion and future research
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Brief History Sad : 1989~90 : Superparticle and Superstring (first-)quantization was attemped.(BV approach) Separation of 1 st Class and 2 nd Class constraints covariantly. Infinitely reducible Constraints. infinite tower of ghosts Happy : 1980’~90’s : 1 st quantized BRST formalism was established. Universal field equation for any spin. Universal free action for any spin. SuperBRST with complete infinite tower of ghosts solved “sad” problem.(still reducible)
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Brink-Schwartz Superparticle action Canonical momenta Primary constraints
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Secondary 1 st class Constraints No cavariant separation of 1 st and 2 nd class constraints in
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Universal field equation for any spin →
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Detouring : 2000 : Pure Spinor formalism Termination in ghost pyramid Complicating composite b ghost Picture changing again Fundamental : 2005 : Direct attack on infinitely reducible 1 st class conts. Fundamental b-c ghosts Arbitrary (S)YM Background Conquest of the ghost pyramid Classical GS superstring action with auxiliary fields
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1 st quantized BRST Adding 2+2 extra unphysical dimensions 2+2 SO(D-1,1) SO(D,2|2) L.C L.C 2+2 SO(D-2) SO(D-1,1|2) Indices : i=(a,α) ; a=(1,...,D) ; α=( , ) ; A=(+,-, α)
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Indices : a=(1,...,D) ; α=( , ) ; A=(+,-, α) OSp(1,1|2) Nonminimal
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minimal nonminimal extension
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Action Spinor
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Examples (1)Vector (2)Spinor
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IGL(1|1) Nonminimal
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Examples Scalar S=0 Spin ½ Vector
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SuperBRST Solved 1 st and 2 nd class constraints problem Complete set of ghosts SYM Background is needed for Superstring
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Technical problem ex) Something is needed to reproduce
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Two different approaches (1)Direct Calculation to have (2)Supersymmetrizing after finding YM b.g (1),(2) give the same result (Constant b.g)
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For arbitrary b.g ‘Big Picture’ like Extended Cohomology Need to shrink Cohomology ex) spin ½
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Superstring (1) should have conformal weight 1 (2)Conformal anomaly should vanish at D=10 (3)X and θ should have conformal weight 0
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Classical superstring action with auxiliary field
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Amplitudes Superparticle Superstring Ghost Pyramid Sum
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Tree amplitude F-1 picture satisfy the same OPE (central charge) due to “ GP sum ”.
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Loop IR regularization Spinor zero mode measure Regularized Spinor propagator
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Rules
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Contractions
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contractions
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Examples 1) Vectors only contractions should give 4pt is the first nonvanishing amplitude 2) Super amplitude – 4pt is the first ex. again
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Conclusion and Future 1 st quantized BRST operator for GS superstring with fundamental b-c ghosts was constructed. Tree and 1 loop amplitudes can be calculated in a manifestly supersymmetric and Lorentz covariant manner. Multiloop amplitude will be calculated. → Geometry is crucial (?)…
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