In general relativity, traversable wormholes are possible provided they do not represent shortcuts in the spacetime. Einstein equations, together with the achronal averaged null energy condition, demand to take longer for an observer to go through the wormhole than through the ambient space. This forbids wormholes connecting two distant regions in the space. The situation is different when higher-curvature corrections are considered. Here, we construct a traversable wormhole solution connecting two asymptotically flat regions, otherwise disconnected. This geometry is an electro-vacuum solution to Lovelock theory of gravity coupled to an Abelian gauge field. The electric flux suffices to support the wormhole throat and to stabilize the solution.In fact, we show that, in contrast to other wormhole solutions previously found in this theory, the one constructed here turns out to be stable under scalar perturbations. We also consider wormholes in AdS. We present a protection argument showing that, while stable traversable wormholes connecting two asymptotically locally AdS 5 spaces do exist in the higher-curvature theory, the region of the parameter space where such solutions are admitted lies outside the causality bounds coming from AdS/CFT. 1 arXiv:1906.02407v2 [hep-th] 30 Jul 2019 1 There have been other interesting papers recently on wormhole geometries; see for instance [14,15,16,17] and references therein and thereof.2 In dimension greater than four, higher-curvature terms do not necessarily yield higher-order terms in the field equations. They can well lead to second-order field equations that are non-linear in the second derivative of the fields.3 The first higher-curvature correction of M theory in 11 dimensions is a quartic term, R 4 [27,28]. When compactifying the theory on a 6-dimensional Calabi-Yau, the effective 5-dimensional theory exhibits R 2 terms as those in (1); see for instance Eqs. (2.6)-(2.9) in [27]; see also Eq. (1) in [29]