Exceptional field theory The U-duality transformations, acting in particular on the generalized metric, then include timelike dualities. It should be emphasized that such dualities, while somewhat unconventional, are of physical interest since they apply whenever one has timelike Killing vectors (or BPS solutions). In addition, theories with a 'Lorentzian generalized metric' are intriguing in that the latter may go through a phase in which the conventional metric components g mn become singular while the generalized metric is still perfectly regular. In this fashion, ExFT encodes truly 'non-geometric' configurations. Another application we will discuss here is the relation to the 'magic tables' that arose in the literature since the early days of supergravity. Specifically, there is an abundance of interesting, often exceptional groups arising in lower dimensions, with various intriguing interrelations and symmetries between them. Here we consider the 'magic triangle' discovered by Cremmer et. al. in compactifications to three dimensions [15]. We will show that the E 8(8) ExFT unifies all theories corresponding to the different entries of that table into a single Lagrangian that, moreover, realises the symmetry of the triangle following a simple group-theory argument. Finally, we review how the generalized type IIB supergravity theory that appeared recently in integrable deformations of AdS/CFT is naturally embedded in ExFT. The rest of this article is organized as follows. In sec. 2 we review ExFT with a focus on the E 6(6) and E 8(8) theories that will be employed later. In sec. 3 we introduce the magic triangle of Cremmer et. al. and explain how it is accommodated within the E 8(8) ExFT. We then turn to timelike dualities and Hull's M *-theories in sec. 4. In sec. 5 we discuss the embedding of generalized IIB supergravity theory, while we close with a brief outlook in sec. 6.