We present a theoretical study of chalcogen bonded container capsules (A_X+A_X) where X=O, S, Se, and Te, and their encapsulation complexes with n‐C₉H₂₀ (n‐C₉H₂₀@A_X+A_X). Both Se and Te encapsulation complexes have significant experimental and computed binding energies, analogous to the hydrogen bonded counterparts, while the S and O capsules and their encapsulation complexes show only weak binding energies, which are attributed to different types of bonding: chalcogen S⋅⋅⋅N bonds for S‐capsules and π–π stacking and weak hydrogen bonds for the O case. All A_X+A_X and C₉H₂₀@A_X+A_X present unusually high magnetic anisotropies in their interiors. The ¹H NMR spectra of the encapsulation complexes display the proton signals of the encapsulated n‐nonane highly upfield shifted, in agreement with the available experimental data for the Se capsule. We found that different factors contribute to the observed magnetic anisotropy of the capsule’s interior: for the Te capsule the most important factor is Te’s large polarizability; for the O analogue the inductive effects produced by the electronegative nature of the O and N heteroatoms; and for the S and Se capsules, the polarizability of the heteroatoms combines with electric field effects.