Fluorescent semiconductor nanoplatelets (epitaxial quantum wells) can be synthesized with excellent monodispersity and self-assembled in highly-ordered structures. Modifications of their electronic and luminescence properties when stacked, due to strong mechanical, electronic or optical interactions between them, have been the topic of intense recent discussions. In this paper, we use Fourier imaging to measure the different dipole components of various nanoplatelet assemblies. By comparing different measurement conditions and corroborating them with polarimetric analysis, we confirm an excellent precision on the dipole components. For single nanoplatelets, only in-plane dipoles (parallel to the platelet plane) are evidenced. For clusters of 2-10 platelets and chains of 30-300 platelets, on the other hand, a clear out-of-plane dipole component is demonstrated. Its contribution becomes more significant as the number of platelets is increased. We review possible explanations and suggest that the added out-of-plane dipole can be induced by strain-induced nanoplatelet deformations.Semiconductor nanoplatelets (NPLs) 1 are quasi-two-dimensional atomically flat nanoemitters with intense, spectrally monodisperse 2 and anisotropic 3-6 emission and potential applications in light-emitting devices 7 , photovoltaic cells 8 , field effect transistors 9 and lasers 10 . Fluorescence studies usually consider, as much as possible, isolated emitters, either by spectroscopy of dilute solutions or by single-molecule microscopy. Interactions between compact assemblies of stacked emitters are however receiving increased attention. In optoelectronics, for instance, these interactions must be understood as they can either be detrimental to a device's efficiency or allow new energy transfer strategies 8,[11][12] . Semiconductor platelets are an ideal model system for studying such interactions because they have a pronounced tendency to spontaneous cofacial stacking [13][14] and because, when stacked, their interactions should be strong as they present high absorption cross-section [15][16] , low Stokes shift and large in-plane dipoles 3,[5][6] which can be aligned parallel at very short distance (2-5 nm) from each other [17][18] . For instance, a second emission peak appears at low temperatures for stacked NPLs and was tentatively attributed to phonon coupling 13 , p-state