The transfer theory of electron microscopy has now been firmly established, at least for the case of axial illumination. Tilted illumination introduces slight complications, but even so the theoretical description of the contrast transfer remains essentially quite simple. Experimentally, the existence of the main "achromatic circle" and the subsidiary circles due to plasmon scattering has been well demonstrated, but the theoretical predictions for the change in the apparent defocus and astigmatism,as determined from the image modified by tilting, has not been confirmed. This paper aims to close the gap.With coherent illumination, the contrast transfer from a weak phase object and for tilted illumination is described by including the beam tilt in the familiar axial expressions:where h(q) is the contrast transfer function (CTF), X(q) the aberration function, and the remaining symbols have their usual meaning. The derivation is algebraically lengthy, but the results can be summarised as follows.