Abstract

This paper presents a worldsheet theory describing holomorphic maps to twistor space with mathcal{N} fermionic directions. The theory is anomaly free when mathcal{N} = 8. Via the Penrose transform, the vertex operators correspond to an mathcal{N} = 8 Einstein supergravity multiplet. In the first instance, the theory describes gauged supergravity in AdS4. Upon taking the flat space, ungauged limit, the complete classical S-matrix is recovered from worldsheet correlation functions.

Highlights

  • The most influential scattering amplitude in Yang-Mills theory is undoubtedly the Parke-Taylor amplitude [1] An,0 =i, j 4 δ4( i pi) 1, 2 2, 3 · · · n, 1 (1.1)It describes the tree-level scattering of two gluons i and j of negative helicity and n − 2 gluons of positive helicity, each of momentum pi = λiλi

  • This paper presents a worldsheet theory describing holomorphic maps to twistor space with N fermionic directions

  • Combining the correlation functions (4.25) & (4.37) with the remaining integral over the zero modes of the Y Z system — i.e., the space of holomorphic maps Z : Σ → PT — and dividing by vol(GL(2; C)) to account for the zero modes of the ghosts associated to the worldsheet gauge theory, we have found that d+2 n d δ2(γ) hi(Z)

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Summary

Introduction

The most influential scattering amplitude in Yang-Mills theory is undoubtedly the Parke-. One outcome of these investigations was given in [32], where it was conjectured that arbitrary n-particle NkMHV tree-level amplitudes in N = 8 supergravity could be represented as This form was obtained by interpreting (1.3) in terms degree 1 holomorphic maps from a Riemann sphere Σ into twistor space, and generalizing to higher degree maps. It is worth pointing out immediately that the present model is more successful than the original twistor strings [12, 56] were (as a theory of pure N = 4 SYM) in at least one respect: the worldsheet correlator we consider leads inexorably to (1.5) and only to (1.5). It seems likely that the relation will be somewhat similar to that between the RNS and pure spinor versions of full string theory [75]

The worldsheet supermanifold
Automorphisms
Deformations
The twistor string
Matter fields
The infinity twistor
BRST transformations
The ghost multiplets
The BRST operator
Worldsheet anomaly cancellation
Zero modes
Vertex operators
Picture changing operators
Scattering amplitudes in the flat space limit
A degenerate infinity twistor
The worldsheet Hodges matrix
The conjugate Hodges matrix
The tree-level S-matrix
Discussion
Higher genus
Boundary correlation functions in AdS4
Other issues
A Some properties of algebraic βγ-systems
Full Text
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