The spin quantum number is defined as 1/2 for particles like electrons due to the eigenvalue equations for spin-1/2 particles, which yield values of ±ħ/2. This choice is not merely conventional; it aligns with the fundamental unit of angular momentum, ħ, and arises from group theory and symmetry principles in quantum mechanics. Spin-1 particles, in contrast, have three eigenvalues (-1, 0, 1), indicating they can exhibit three observable states. The concept of spin does not imply actual rotation; rather, it reflects the behavior of the Dirac wavefunction under coordinate transformations. Ultimately, the definition of spin is rooted in the symmetries of quantum mechanics rather than physical rotation.