“…119 Sn is the most suitable tin isotope for NMR experiments because among the three spin I = 1/2 isotopes ( 115 Sn, 117 Sn and 119 Sn) it has the highest sensitivity. However, being a heavy atom, it usually manifests large magnetic shielding anisotropies and in conducting and semiconducting materials it is also affected by the hyperfine interaction with free electrons, which can shift and broaden the signals and strongly shorten the spin–lattice relaxation time T 1 . − These interactions, which can heavily broaden the SSNMR peaks together with the relatively low 119 Sn sensitivity, often make 119 Sn SSNMR experiments quite challenging. Moreover, working on NCs induces further peak-broadening effects, since the nanosize and the high surface-to-volume ratio make surface effects particularly important. ,, Nevertheless, 119 Sn SSNMR proved to be very successful in investigating the structural and electronic properties of complex conducting and semiconducting materials. ,− As far as ITO is concerned, while several structural models, for bulk or films, have been proposed, , only a few experimental studies, based on 119 Sn Mössbauer spectroscopy, XRD, EXAFS, neutron diffraction, and SSNMR, have been reported in the literature. ,,− …”