Abstract

We compute one-loop threshold corrections toℛ4terms inN=5,6supergravity vacua of Type II superstrings. We then discuss nonperturbative corrections generated by asymmetric D-brane instantons. Finally we derive generating functions for MHV amplitudes at tree level inN=5,6supergravities.

Highlights

  • N 5, 6 supergravities in D 4 enjoy many of the remarkable properties of N 8 supergravity

  • The threshold corrections that we find may be taken as evidence that, as in the N 8 case, superstring calculations do not reproduce field theory results, where such R4 corrections are absent as a result of the unbroken anomaly free continuous U-duality symmetry as in the N 8 case 1

  • Since N 5, 6 supergravities can be obtained as asymmetric orbifolds of tori, tree-level scattering amplitudes of untwisted states such as gravitons are identical to the corresponding amplitudes in the parent N 8 theory

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Summary

Introduction

N 5, 6 supergravities in D 4 enjoy many of the remarkable properties of N 8 supergravity. The threshold corrections that we find may be taken as evidence that, as in the N 8 case, superstring calculations do not reproduce field theory results, where such R4 corrections are absent as a result of the unbroken anomaly free continuous U-duality symmetry as in the N 8 case 1. This is in line with the nondecoupling in Type II superstrings of BPS states that are singular from the strict 4-dimensional supergravity perspective 8–10. We will only focus on R4 terms in D 4 the parent D 5 theory is instrumental to the identification of the relevant BPS instantons

N 6 2L 4R Supergravity in D 5
N 6 Supergravities in D 4
N 5 1L 4R Supergravity in D 4
Four-Graviton One-Loop Amplitude
Td gs2
H urs 6 H urs
World-Sheet Integrations
One-Loop Threshold Integrals
Low-Energy Action and U-Duality
N 6 ED-Branes
Nonperturbative Threshold Corrections
N 5 ED-Branes
Conclusions
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