“…Here, we use 15 N spin–lattice relaxation attributed to the 15 N– 1 H magnetic dipolar interaction as a direct tool for observation of the proton (hydrogen) location and dynamics, i.e., the PT rate. The 15 N– 1 H magnetic dipolar interaction in the solid state has often been applied to analyze the structures of hydrogen-bond systems including nitrogen atom(s) because of the inverse cubic dependence of the magnitude of the local magnetic field by the nuclear spins, such as protons, near the 15 N nucleus. − In solution, on the other hand, the dynamics of the molecules, e.g., the reorientational motion, causes the 15 N– 1 H dipolar interaction to fluctuate, so that the 15 N spin–lattice relaxation time attributed to the 15 N– 1 H magnetic dipolar interaction, T 1 dd ( N H), depends on the correlation time of the reorientation of the NH vector. , The T 1 dd ( N H) value is also dependent on the PT dynamics, because the PT, i.e., the proton jump, causes the NH distance to fluctuate. The contribution of the PT dynamics to the spin–lattice relaxation induced by the magnetic dipolar interaction in solution has already been discussed in detail. , In the present paper, we attempt to determine the proton location and its dynamics, i.e., the PT rates, for the chosen Schiff bases in dichloromethane and acetonitrile solutions from the 15 N spin–lattice relaxation times, taking into account the NH reorientational motions.…”