Van der Waals (vdW) interfaces based on two dimensional (2D) materials are promising for optoelectronics, as interlayer transitions between different compounds allow tailoring the spectral response over a broad range. However, issues such as lattice mismatch or a small misalignment of the constituent layers can drastically suppress electron-photon coupling for these interlayer transitions.Here, we engineer type-II interfaces by assembling atomically thin crystals that have the bottom of the conduction band and the top of the valence band at the Γ-point, thus avoiding any momentum mismatch. We find that these vdW interfaces exhibit radiative optical transitions irrespective of lattice constant, rotational/translational alignment of the two layers, or whether the constituent materials are direct or indirect gap semiconductors. Being robust and of general validity, our results broaden the scope of future optoelectronics device applications based on two-dimensional materials. Van der Waals interfaces of interest for optoelectronics consist of two distinct layered semiconductors with a suitable energetic alignment of their conduction and valence bands, such that electron and hole excitations reside in the two separate layers.[1-4] This allows the interfacial band gap to be controlled by material selection -as well as by application of an electrical bias or strain[5-9]-so that electron-hole recombination across the layers generates photons with frequency determined over a broad range at the design stage. Choosing the interface components among the vast gamut of 2D materials -including semiconducting transition metal dichalcogenides (TMDs, MoS 2 , MoSe 2 , MoTe 2 , WS 2 , WSe 2 , ReS 2 , ZrS 2 , etc.), III-VI compounds (InSe, GaSe), black phosphorous, and even magnetic semiconductors (CrI 3 , CrCl 3 , CrBr 3 , etc.)-enables, at least in principle, to cover a spectral range from the far infra-red to the violet. In practice, however, efficient light-emission from interlayer recombination requires the corresponding electron-hole transition to be direct in reciprocal (k-) space: the bottom of the conduction band in one layer has to be centered in k-space at the same position as the top of the valence band in the other layer.[10] This requirement poses severe constraints as concluded from heterostructures of monolayer semi-conducting TMDs, the systems that have been so far mostly used to realize light-emitting vdW interfaces. [7,[11][12][13][14] Indeed, in this case the minimum of the conduction band and top of valence band are at the K/K' points in the Brillouin zone and the presence of radiative