Its interaction with itself explains why two neighboring protons split an NMR signal into a triplet, while four neighboring protons split it into a quartet. It decouples from the orbit in the Paschen-Back effect, and its interaction with the orbital angular momentum dominates in light atoms and is known as Russell-Saunders coupling. The Dirac equation governs the relativistic behavior of particles with a value of one-half for this quantity, and particles with integral va
Its interaction with itself explains why two neighboring protons split an NMR signal into a triplet, while four neighboring protons split it into a quartet. It decouples from the orbit in the Paschen-Back effect, and its interaction with the orbital angular momentum dominates in light atoms and is known as Russell-Saunders coupling. The Dirac equation governs the relativistic behavior of particles with a value of one-half for this quantity, and particles with integral values of it are governed by Bose-Einstein statistics. First proposed by Uhlenbeck and Goudsmitt and verified by the Stern-Gerlach experiment, for 10 points, identify this intrinsic angular momentum of particles.
Its interaction with itself explains why two neighboring protons split an NMR signal into a triplet, while four neighboring protons split it into a quartet.
{spin} angular momentum