One-dimensional harmonic oscillator:
1D Harmonic Oscillator + Electric Field
Problem: Analyze the effect of an electric field on a 1D harmonic oscillator and compare two approaches:
- Perturbation Theory: Estimates energy shifts and dipole moment for weak fields.
- Exact Solution: Provides precise results but can be more challenging to find.
1. Perturbation calculation:
- Hamiltonian: H = H₀ - ezE (unperturbed + perturbation)
- Energy shifts to second order:
- ΔE_n^(2) = - |<n|ez|m>|<^2 / (E_n - E_m) (sum over m ≠ n)
- Induced dipole moment: p = -e <z> ≈ -e∑_n ρ_n <n|z|n>
2. Exact solution:
- Hamiltonian: H = -ħ²/2m d²/dz² + 1/2 mω²z² - ezE
- Solve Schrödinger equation: Obtain exact energy eigenvalues and eigenfunctions.
- Compare with perturbation results: Verify accuracy of perturbation approximation.
3. Three-dimensional isotropic oscillator:
- Hamiltonian: H = H₀ - eEz (z-component of perturbation)
- Energy shifts and dipole moment: Calculate analogously to 1D case.
- Polarizability: α = p/E = -e∑_n ρ_n <n|z|n> / E
- Energy shift: ΔE = -1/2 αE² (holds exactly for isotropic oscillator)
Key points:
- Perturbation theory: Estimates energy shifts and dipole moments for weak perturbations.
- Exact solution: Possible for some cases, providing a benchmark for perturbation results.
- Polarizability: Relates induced dipole moment to electric field strength.
- Isotropic oscillator: Has a specific polarizability expression and energy shift formula.