Bum-Hoon Lee Sogang University, Seoul, Korea D-branes in Type IIB Plane Wave Background 15th Mini-Workshop on Particle Physics May 14-15, 2006, Seoul National University
Based on the works: 1. J. Kim, BHL, & H.S. Yang Superstrings and D-branes in A Plane Wave Phys. Rev. D68 (2003) , hep-th/ K.-S. Cha, BHL, & H.S. Yang Intersecting D-branes in IIB PP Background Phys. Rev.D68 (2003) , hep-th/ K.-S. Cha, BHL, & H.S.Yang Supersymmetric D-branes in IIB PP Background JHEP03 (2004) 058, hep-th/ BHL,Jong-won Lee, Chanyong Park, HyunSeok Yang More on supersymmetric D-branes in type IIB plane wave background JHEP 01 (2006) 015, hep-th/ References Center for Quantum Spacetime
* pp waves as limits of the metric of Consider the geometry near the trajectory of a particle that is moving along the direction and sitting at and - introducing new coordinates - performing the following rescaling then, we obtain
Rewrite this as the form of pp wave metric The mass parameter is introduced by rescaling In global coordinates in energy : angular momentum : In terms of the dual CFT, these are the conformal dimension and R- charge of a state of the field theory on where the has unit radius.
Some relation * Strings on pp-waves Choose light-cone gauge ; ( is the worldsheet time.) The light-cone action
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pp-wave background metric
- the light-cone Hamiltonian : From the point of view, is given by
* Strings from N=4 Super Yang-Mills In the limit find the spectrum of states with finite (single trace states of the Yang-Mills theory on - Taking to be the generator rotating the plane 56, the vacuum state in light-cone gauge (corresponding to a unique single trace operator with ) is - 8 bosonic and 8 fermionic modes with On the string theory side, we construct all these states by applying the zero momentum oscillators to and on the light-cone vacuum
* Strings from N=4 Super Yang-Mills In the limit find the spectrum of states with finite (single trace states of the Yang-Mills theory on - Taking to be the generator rotating the plane 56, the vacuum state in light-cone gauge (corresponding to a unique single trace operator with ) is
- 8 bosonic and 8 fermionic modes with On the string theory side, we construct all these states by applying the zero momentum oscillators to and on the light-cone vacuum These string states correspond to the following operators in the Super Yang-Mills theory
* Dp-brane in the pp wave background Start with the pp wave metric and 5-form flux This background is maximally supersymmetric and thus preserve 32 supersymmetries.
In the light-cone gauge, the Green-Schwarz action is : Equations of motion for string
Boundary conditions for boson Neunmann : Dirichlet : for fermion For BPS objects that preserve 16 supersymmetries, have to satisfy two conditions - 1 st condition -> allows only odd p branes
Center for Quantum Spacetime Boundary Open string Bulk Closed string + Open string sector D5-D5 + D3-D5 string D3 ½ BPS (# 16 SUSY) D5 D-branes Intersecting # N SUGRA Solution Ads_5 X S^5 N=4 d=3+1 SYM Near Horizon limit Conformal limit
Center for Quantum Spacetime BMN limit N=4 d=3+1 SYM (λ=g YM ^2, N<<1) 2+1 dim defect CFT Penrose limit Max. SUSY # 32 Ads_5 X S^5 (g s N >> 1) Ads_4 X S^2, D brane Intersecting (J, Δ>>1) Sector of SYM λ’ = g YM ^2 N / J^2 G. Semenoff … Constable … Corresponding dCFT Max. SUSY # 32 Symmetric Plane Wave Geometry Blau, … Metsaev … D-branes : Open string sector Intersecting
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Ex) Flat Minkowski Center for Quantum Spacetime IIB ½ BPS : D1 D3 D5 D7 D9 Dp-braneIntersectin D-branes Dp-Dp’ # ND, DN = 0, 4, 8 : SUSY If Not, NO SUSY D1 D3 Dp-DpD(p+4) Dp ¼BPS :
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The allowed choices for Solutions for bosonic coordinates
for fermions The boundary conditions
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Summary Supersymmetric intersecting D-brane configurations intersecting D-brane configurations in pp-wave background in pp-wave background are systematically classified are systematically classified Dual field theories and Application to the Phenomenological Model buildings to be Phenomenological Model buildings to be studied studied Center for Quantum Spacetime