Most known vanadium(V) complexes with redox-active o-dioxolene ligands are non-innocent. Since the vanadium(V) complex [VO(gsal)(HCat)] is innocent, its properties were investigated by 51 V solid-state NMR spectroscopy and density functional theory (DFT). The innocent ligand behavior manifested itself by the upfield isotropic chemical shift and large negative chemical shift anisotropy observed in the solid state. The electronic structure and NMR spectroscopic parameters of this complex were addressed by DFT calculations and found to be consistent with the NMR spectroscopic observa-4646 asymmetry parameter (δ σ , η σ ), together with the relative quadrupolar and CSA tensor orientations described by the Euler angles (α, β, γ) were extracted by numerical simulations of the full manifold of the spinning sidebands corresponding to the central and satellite transitions with the SIMPSON [30] software package. The best-fit parameters are summarized in Table 1.In this work, we use the Haeberlen-Mehring-Spiess convention to define the CSA tensor elements, [14] where |δ xx -δ iso | Յ |δ yy -δ iso | Յ |δ zz -δ iso |, δ iso = (δ xx + δ yy + δ zz )/3, δ σ = δ zz -δ iso , and η σ = (δ yyδ xx )/(δ zz -δ iso ). In this representation, δ ii corresponds to the principal components of the chemical shift tensor. The electric field gradient (EFG) tensor parameters are defined as C Q = eQV ZZ /h and η Q = (V XX -V YY )/V ZZ where |V ZZ | Ն |V YY | Ն |V XX |, e is the electronic charge, and h is Planck's constant.DFT Calculations: Quantum chemical calculations of the NMR spectroscopic parameters for [VO(gsal)(HCat)] and the hypothetical deprotonated complex [VO(gsal)(Cat)]were performed with DFT in Gaussian09. [31] The 51 V magnetic shielding and EFG tensors for both molecules were computed by using B3LYP and BLYP functionals. [32][33][34] For each method, calculations were conducted with three basis sets: (i) 6-311+G, (ii) TZV, [35] and (iii) augmented Wachters basis set on V [36,37] and 6-31* [38][39][40] on all other elements. Calculations were carried out by using geometry-optimized structures at the B3LYP/TZV level, and the Cartesian coordinates for the geometry-optimized [VO(gsal)(HCat)] and [VO(gsal)(Cat)]are presented in Table 1. The nuclear magnetic shielding calculations