Stark Effect
The Stark effect is the splitting or shifting of quantum energy levels in an applied electric field. The basic perturbation is electric-dipole coupling, but the observed response depends on parity, degeneracy, polarizability, and whether the field is static or oscillatory.
Formula Hook
Section titled “Formula Hook”For a static electric field,
For a nondegenerate stationary state , first-order perturbation theory gives
If parity makes the first-order shift vanish, the leading static shift is often written
where is the polarizability in the chosen convention.
Canonical Home
Section titled “Canonical Home”This glossary entry is the named-effect home. Stark Effect as a Perturbation Example owns the static method choice, polarizability check, and ideal-hydrogen calculation. Stark Effect in Atoms owns scalar, vector, and tensor polarizabilities, AC shifts, traps, and spectroscopy. For adjacent examples and concepts, see Rotor in External Fields: First Encounter, Degeneracy Lifting, Nondegenerate Perturbation Theory, and Degenerate Perturbation Theory.
Common Confusions
Section titled “Common Confusions”- A first-order Stark shift vanishes for many nondegenerate parity eigenstates, but not for every system.
- Degenerate hydrogen has a linear Stark effect because the perturbation mixes degenerate opposite-parity states.
- The AC Stark effect is a driven, frequency-dependent light-shift problem, not just the DC formula with a time-varying field inserted.
- Polarizability signs and factors of depend on the energy convention being used.
Related Entries
Section titled “Related Entries”- Eigenstate
- Amplitude
- Degeneracy Lifting
- Stark Effect as a Perturbation Example
- Stark Effect in Atoms
- Zeeman Effect
References
Section titled “References”- C. Cohen-Tannoudji, B. Diu, and F. Laloe, Quantum Mechanics, Wiley, 1977.
- C. J. Foot, Atomic Physics, Oxford University Press, 2005.
- D. J. Griffiths and D. F. Schroeter, Introduction to Quantum Mechanics, 3rd ed., Cambridge University Press, 2018.