NMR chemical shift tensors (CSTs) in proteins, as well as their orientations, represent an important new restraint class for protein structure refinement and determination. Here, we present the first determination of both CST magnitudes and orientations for 13 Cα and 15 N (peptide backbone) groups in a protein, the β1 IgG binding domain of protein G from Streptococcus spp., GB1. Site-specific 13 Cα and 15 N CSTs were measured using synchronously evolved recoupling experiments in which 13 C and 15 N tensors were projected onto the 1 H-13 C and 1 H-15 N vectors, respectively, and onto the 15 N-13 C vector in the case of 13 Cα. The orientations of the 13 Cα CSTs to the 1 H-13 C and 13 C-15 N vectors agreed well with the results of ab initio calculations, with an rmsd of approximately 8°. In addition, the measured 15 N tensors exhibited larger reduced anisotropies in α-helical versus β-sheet regions, with very limited variation (18 AE 4°) in the orientation of the z-axis of the 15 N CST with respect to the 1 H-15 N vector. Incorporation of the 13 Cα CST restraints into structure calculations, in combination with isotropic chemical shifts, transferred echo double resonance 13 C-15 N distances and vector angle restraints, improved the backbone rmsd to 0.16 Å (PDB ID code 2LGI) and is consistent with existing X-ray structures (0.51 Å agreement with PDB ID code 2QMT). These results demonstrate that chemical shift tensors have considerable utility in protein structure refinement, with the best structures comparable to 1.0-Å crystal structures, based upon empirical metrics such as Ramachandran geometries and χ 1 ∕χ 2 distributions, providing solid-state NMR with a powerful tool for de novo structure determination.magic-angle spinning | dihedral angles | cross validation | nanocrystal | quantum chemistry T he chemical shift is an exquisite and powerful probe of molecular structure, deriving from the interaction of molecular orbitals with an external magnetic field, B 0 . Understanding the relationships between chemical shifts and protein structure has substantial implications for modern nuclear magnetic resonance (NMR) spectroscopy, chemistry, and structural biology (1-12). The chemical shift tensor (CST) is rich with information, even when two-thirds of it is averaged to zero by molecular tumbling in solution or magic-angle spinning (MAS) of solid samples. The remaining isotopic chemical shifts remain an excellent resource for structure determination and validation, and higher-order interactions of the CST have substantial contributions to NMR relaxation (13-19). Therefore, detailed knowledge of CSTs permits a precise analysis of motion (20)(21)(22). Solid-state NMR (SSNMR) of fully aligned samples exploits amide 15 N tensor information to determine the orientations of helices relative to the bilayer (23, 24). We have previously shown that use of a force field in which experimental 13 Cα CSTs are compared with ab initio CSTs [generated as a function of backbone conformation (ϕ, ψ)] significantly improves the precision and...