The electron is predicted to be slightly aspheric [1], with a distorsion characterised by the electric dipole moment (EDM), d e . No experiment has ever detected this deviation. The standard model of particle physics predicts that d e is far too small to detect [2], being some eleven orders of magnitude smaller than the current experimental sensitivity. However, many extensions to the standard model naturally predict much larger values of d e that should be detectable [3]. This makes the search for the electron EDM a powerful way to search for new physics and constrain the possible extensions. In particular, the popular idea that new supersymmetric particles may exist at masses of a few hundred GeV is difficult to reconcile with the absence of an electron EDM at the present limit of sensitivity [4,2]. The size of the EDM is also intimately related to one 1