(I) Property of all nuclei related to the largest measurable component of the nuclear
angular momentum. Non-zero values of nuclear
angular momentum are quantized (fixed) as
integral or half-integral multiples of (h/2p), where h is Planck's constant. The number of possible
energy levels for a given
nucleus in a fixed
magnetic field is equal to 2I + 1. Similarly, an unpaired electron has a
spin of 1/2 and two possible
energy levels.