The Stern-Gerlach experiment demonstrates the quantization of electron spin by passing a beam of atoms through a non-uniform magnetic field, leading to discrete splitting.
- It is mainly observed with atoms having non-zero total angular momentum.
- Atoms in the \( 2S_{1/2} \) state exhibit the expected behavior.
- However, the \( 1S_0 \) state corresponds to **zero total angular momentum**, meaning it does not exhibit Stern-Gerlach splitting.