world-sheet scattering in ads 5 xs 5
DESCRIPTION
World-sheet Scattering in AdS 5 xS 5. Konstantin Zarembo (Uppsala U.). T.Klose, T.McLoughlin, R.Roiban, K.Z., hep-th/0611169 T.Klose, K.Z., hep-th/0701240 T.Klose, T.McLoughlin, J.Minahan, K.Z., 0704.3891. Random Matrix Theory: Recent Applications, Copenhagen, 14.05.07. - PowerPoint PPT PresentationTRANSCRIPT
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World-sheet Scattering in AdS5xS5
Konstantin Zarembo(Uppsala U.)
Random Matrix Theory: Recent Applications, Copenhagen, 14.05.07
T.Klose, T.McLoughlin, R.Roiban, K.Z., hep-th/0611169T.Klose, K.Z., hep-th/0701240T.Klose, T.McLoughlin, J.Minahan, K.Z., 0704.3891
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AdS/CFT correspondence Maldacena’97
Gubser,Klebanov,Polyakov’98Witten’98
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Anti-de-Sitter space (AdS5)
5D bulk
4D boundary
z
0
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Sigma-model in AdS5xS5:• well-defined theory with the known (but
complicated) Lagrangian• also integrable!• Exactly solvable?• How does the (discrete) spin chain arise from
the (continuous) world-sheet?
Spectral problem in large-N SYM:• can be reformulated in terms of an integrable spin
system
Bena,Polchinski,Roiban’03
Minahan,Z.’02Beisert,Kristjansen,Staudacher’03Beisert,Staudacher’03
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The non-perturbative S-matrix for the spin chain is known*
Goal: check if the same S-matrix describes scattering on the world sheet
Beisert’05Beisert,Eden,Staudacher’06
*) But the Hamiltonian is not!
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Sigma-model in AdS5xS5Metsaev,Tseytlin’98
Sigma-model coupling constant:
Classical limitis
Green-Schwarz-type coset PSU(2,2|4)/SO(4,1)xSO(5)
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φ
yi’
t
zi
S5 AdS5
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The metric
AdS5 S5
Transverse coordinates:
+ RR flux
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Fermion part of the sigma-model is of Green-Schwarz type.
Conformal gauge is problematic:• no kinetic term for fermions • no holomorphic factorization for currents, …
RR flux requires manifest space-time supersymmetry
Standard CFT does not work…
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Kinetic term for fermions:
If X=const, ρa=0 and the kinetic term vanishes.
Need to fix the light-cone gauge: X+=τ(then ρ0=Γ+ and the kin. term is not degenerate)
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Gauge fixing
Light-like geodesics:
angular momentum
Berenstein,Maldacen,Nastase’02Parnachev,Ryzhov’02Callan,Lee,McLoughlin,Schwarz,Swanson,Wu’03Arutyunov,Frolov,Plefka,Zamaklar’06
Gubser,Klebanov,Polyakov’02
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Unbroken bosonic subgroup:
Taking into account supersymmetry:
This also gets central extension with
p – world-sheet momentum
Beisert’05Arutyunov,Frolov,Plefka,Zamaklar’06
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World-sheet fields
World-sheet fields (embedding coordinates in AdS5xS5):
global time in AdS5 and angle on S5 – eliminated by gauge condition
Fields form (2|2)x(2|2) multiplet of PSU(2|2)2:
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Gauge-fixed action
Loop counting parameter:
Internal string length:
Decompatification (infinite string) limit:
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Gauge-fixed Lagrangian (the bosonic part):
is the gauge parameter
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Bosonic Lagrangian up to quartic order in fields:
• Massive, integrable 2d field theory• Lorentz invariant kin. terms• Lorentz invariance is broken by interactions• Gauge-dependent: a=1/2 (pure l.c. gauge) is the
simplest case
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World-sheet scattering
S-matrix:
Integrability (consistency with Yang-Baxter equations) requires:
SU(2)4 – invariace:
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Tree level
SU(2)4 form of T:
Klose,McLoughlin,Roiban,Z.’06
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Beisert’05
Coincides with the expansion of the spin-chain S-matrix:(gauge dependence affects only the overall phase)
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Dressing phase
To leading order in :Beisert,Hernandez,Lopez’06Beisert,Eden,Staudacher’06
agrees with tree-levelscattering amplitudes in the sigma-model
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Near-flat limitMaldacena,Swanson’06
perturbative string modes
giant magnons Hofman,Maldacena’06talk by Semenoff
“Left-moving” sector:
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Reduced Sigma Model
Consistent truncation of the full sigma-model:
Maldacena,Swanson’06
- chiral SO(8) spinor
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Dispersion relation
Exact dispersion relation:
In the near-flat limit:
At λ→∞:
Mass receives radiative corrections starting from two loops
(exact)
Beisert,Dippel,Staudacher’04
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Tadpole cancellation
+ = 0
= 0
Yi’ (S5) Zi (AdS5)
(fermions)
The same mechanism renders the model finiteto any order in perturbation theory
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Mass renormalization
=
Mass-shell condition:
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S-matrix
One loop:
Two loops:
+ mass renormalization+ two-loop corrections to Z-factors
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Tree-level amplitude:
One-loop correction:
Klose,Z.’07
Two loops:
Klose,McLoughlin,Minahan,Z.’07
Agrees!
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“Lorentz-invariant” form of the S-matrix
All Lorentz non-invariance of amplitudes in the reduced model can behidden in the momentum-dependent redefinition of the coupling:
In the full σ-model/spin chain, LI is possibly q-deformed rather than violated Gomez,Hernandez’06; Young’07
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Conclusions
• At strong coupling, the SU(2|2)xSU(2|2) S-matrix describes the scattering of the string modes in the light-cone gauge
• Perturbative calculations of scattering amplitudes agree with the conjectured BHL/BES phase up to two loops at strong coupling (and to four loops at week coupling Bern,Czakon,Dixon,Kosower,Smirnov’06)
• Ultimately we want to quantize the σ-model with periodic bounary conditions, when S-matrix is not well defined.
• S-matrix → asymptotic Bethe ansatz• ???????? → exact Bethe ansatz
talk by Staudacher