I. Introduction
Electron tomography is a powerful tool in materials science to characterize the complex three-dimensional (3D) structure of inorganic specimens on the nanoscale [1]. In transmission electron microscopy (TEM), the sample under study is exposed to an electron beam and tilted to obtain two-dimensional (2D) projection images at different angles. Several imaging modalities exist, e.g., bright-field TEM [2] and high-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) [3]. In tomography, these projections are called a tilt-series, from which we can reconstruct a volume representing the sample [1]. Since the intensity of HAADF-STEM scales with the atomic number of the element (, , depending on the inner and outer detector angles [4]), it can also indirectly reveal the compositional information of the sample. However, when the sample has elements with close atomic numbers, HAADF-STEM images may no longer be distinctive for these elements. To better understand more complex compositions, spectral imaging techniques like energy dispersive X-ray spectroscopy (EDS) [4] must be pursued.