Abstract

We study the space of all kinematically allowed four photon and four graviton S-matrices, polynomial in scattering momenta. We demonstrate that this space is the permutation invariant sector of a module over the ring of polynomials of the Mandelstam invariants s, t and u. We construct these modules for every value of the spacetime dimension D, and so explicitly count and parameterize the most general four photon and four graviton S-matrix at any given derivative order. We also explicitly list the local Lagrangians that give rise to these S-matrices. We then conjecture that the Regge growth of S-matrices in all physically acceptable classical theories is bounded by s2 at fixed t. A four parameter subset of the polynomial photon S-matrices constructed above satisfies this Regge criterion. For gravitons, on the other hand, no polynomial addition to the Einstein S-matrix obeys this bound for D ≤ 6. For D ≥ 7 there is a single six derivative polynomial Lagrangian consistent with our conjectured Regge growth bound. Our conjecture thus implies that the Einstein four graviton S-matrix does not admit any physically acceptable polynomial modifications for D ≤ 6. A preliminary analysis also suggests that every finite sum of pole exchange contributions to four graviton scattering also violates our conjectured Regge growth bound, at least when D ≤ 6, even when the exchanged particles have low spin.

Highlights

  • 1.1 Motivation Consider a compactification of Type II string theory on Rp × M10−p.1 The string spectrum on this background includes four dimensional gravitons

  • A preliminary analysis suggests that every finite sum of pole exchange contributions to four graviton scattering violates our conjectured Regge growth bound, at least when D ≤ 6, even when the exchanged particles have low spin

  • We argue that all such contributions to four graviton scattering appear to violate the Classical Regge Growth (CRG) bound at least for D ≤ 6

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Summary

Introduction

1.1 Motivation Consider a compactification of Type II string theory on Rp × M10−p.1 The string spectrum on this background includes four dimensional gravitons. There are no poles from the exchange of particles outside the sector CpII These facts — which follow immediately from the general structure of string worldsheet perturbation theory (see appendix A.1)- have a striking target space interpretation. In the limit gs → 06 graviton scattering amplitudes for type II/ Heterotic theory on Rp × M10−p reduce to the tree amplitudes computed using S(CpII) or S(CpH). Conjecture 1: there exist exactly three classical gravitational S-matrices that are consistent with a set of physically motivated ‘low energy’ constraints (including stability of the vacuum, factorization on poles, causality and positivity of energy) These are the Einstein S-matrix generated by SEinstein, the type II S-matrix generated by S(CpII) and the Heterotic S-matrix generated by S(CpH). This is the same regime of applicability as [2]

Three graviton scattering
A conjectured bound on Regge scattering
Consequences of the CRG conjecture
Polynomial amplitudes
Exchange contributions
Organization of this paper
Momenta
Polarizations
Unconstrained polarizations
S4 permutation symmetry
Action of permutations on unconstrained data
Effective transformations under permutations
Permutations
Local S-matrices and a module structure
The local module
The bare module
Embedding the local module into the bare module
Irreducible representations of S3 and fusion rules
Projecting onto S3 singlets
Standard bases for representations of S3
Counting S-matrices
2.10 Regge growth
Generators of the bare module
Enumeration
Explicit construction of eI and S3 transformations
Local Lagrangians and local S-matrices
Scalars
Photons
Gravitons
Polynomial photon S-matrices and corresponding Lagrangians
Explicit expressions for most general S-matrix and corresponding Lagrangians
Polynomial graviton S-matrices and corresponding Lagrangians
Discussion

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