Skyrmions [1] are topologically non-trivial vortex-like spin textures, anticipated for application in spintronic technologies, in next generation magnetic data processing and storage due to their facile manipulation by spin-polarized currents of very low magnitude [2,3]. Unfortunately, little is known about the 3D structure of skyrmions [4,5], ubiquitous in thin film technology. Here, we bridge that gap by combining the concept of the transport of intensity equation (TIE) [6], focal series in-line electron holography (EH), and off-axis EH [7] to quantitatively reconstruct the projected magnetic field pertaining to both the helical and the skyrmion lattice phase in single crystal nanoparticles of the isotropic chiral magnet Fe0.95Co0.05Ge.The skyrmion phase in Fe0.95Co0.05Ge particles ( Fig. 1 (b)) was investigated using a double corrected FEI Titan³ 80-300 microscope operated in image corrected Lorentz mode. A focal series of Lorentz TEM (L-TEM) images of a single isolated nanoplatelett oriented along the [001] zone axis ( Fig. 1 (a)) was recorded. Reconstruction of the phase of the electron wave and thereby of the magnetic induction was obtained with the help of a modified Gerchberg-Saxton type algorithm. To supplement the focal series reconstructions from large field of views, smaller areas of the identical nanoplatelett were investigated by off-axis EH. A direct tomographic investigation of the 3D structure of the skyrmionic lattice is currently experimentally unfeasible, because this would require an externally applied out-ofplane magnetic field to be tilted with the sample. Thus, indirect experimental evidence for the 3D structure of the skyrmionic lattice may currently only be inferred from a quantitative analysis of the projected magnetic induction in the sample conducted with the help of EH. Fig. 2 (a) depicts an underfocused L-TEM micrograph showing the hexagonal that reveals the skyrmion lattice. The image is one out of 21 of the focal series used for an in-line holography reconstruction of the object exit wave in amplitude and phase. Figs. 2 (b, c) show magnetic induction maps " # ( , ) in cylindrical coordinate representation visualizing the spin texture of the skyrmions by " * ( , ) (Fig. 2(b)) and their donut-shaped magnitude by " + ( , ) (Fig. 2 (c)). Likewise, we observed magnetic induction maps (Figs. 2 (e, f)) from a phase image reconstructed by off-axis EH (Fig. 2(d)) on the same Fe0.95Co0.05Ge nanoplatelett. Most strikingly, we consistently observe a reduction of the projected in-plane B-fields ( " ,-. = (0.2 . . . 0.3) ) as compared to those of a homogeneous skyrmion throughout the film thickness. Two alternative models for the 3D structure of skyrmions are thus derived.