Ambitwistor strings are chiral (holomorphic) strings whose target is the space of complex null geodesics, ambitwistor space. We introduce twistor representations of ambitwistor space in 6 and 5 dimensions. In 6d the twistor representation is naturally conformally invariant. Anomaly cancellation leads to models that describe biadjoint scalar amplitudes and certain conformally invariant gauge and gravity theories, respectively of 4th and 6th order. There are three such models, reflecting triality for the conformal group SO(8) associated to these 6d models. On reduction to five dimensions, gauge anomaly cancellation requires supersymmetry and the resulting models describe maximally supersymmetric Yang-Mills and gravity. The twistor representat...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
Abstract: Ambitwistor strings are chiral (holomorphic) strings whose target is the space of complex ...
Abstract Ambitwistor strings are chiral (holomorphic) strings whose target is t...
We begin with an overview of the scattering equations, CHY formalism and the ambitwistor string. We ...
Tree-level scattering amplitudes in massless theories not only exhibit a simplicity entirely unexpec...
Tree-level scattering amplitudes in massless theories not only exhibit a simplicity entirely unexpec...
We introduce a spinorial version of the scattering equations, the \emph{polarized scattering equatio...
We obtain compact formulae for tree super-amplitudes for 10 and 11-dimensional supergravity and 10-d...
We show that string theories admit chiral infinite tension analogues in which only the massless part...
The physical states of N=4 conformal supergravity in four dimensions occur in twistor-string theory ...
We reformulate twistor-string theory as a heterotic string based on a twisted (0, 2) model. The path...
We introduce a spinorial version of the scattering equations, the \emph{polarized scattering equatio...
We reformulate twistor-string theory as a heterotic string based on a twisted (0,2) model. The path ...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
Abstract: Ambitwistor strings are chiral (holomorphic) strings whose target is the space of complex ...
Abstract Ambitwistor strings are chiral (holomorphic) strings whose target is t...
We begin with an overview of the scattering equations, CHY formalism and the ambitwistor string. We ...
Tree-level scattering amplitudes in massless theories not only exhibit a simplicity entirely unexpec...
Tree-level scattering amplitudes in massless theories not only exhibit a simplicity entirely unexpec...
We introduce a spinorial version of the scattering equations, the \emph{polarized scattering equatio...
We obtain compact formulae for tree super-amplitudes for 10 and 11-dimensional supergravity and 10-d...
We show that string theories admit chiral infinite tension analogues in which only the massless part...
The physical states of N=4 conformal supergravity in four dimensions occur in twistor-string theory ...
We reformulate twistor-string theory as a heterotic string based on a twisted (0, 2) model. The path...
We introduce a spinorial version of the scattering equations, the \emph{polarized scattering equatio...
We reformulate twistor-string theory as a heterotic string based on a twisted (0,2) model. The path ...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...
We consider D-dimensional amplitudes in R-2 gravities (conformal gravity in D = 4) and in the recent...