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Advanced Quantum Mechanics

Manual: General · Subject: Quantum Mechanics

Perturbation theory, variational method, and scattering

Approximation Methods in Quantum Mechanics

Time-Independent Perturbation Theory

When H=H0+λH′H = H_0 + \lambda H' (λ≪1\lambda \ll 1), first-order energy correction:<br>En(1)=⟨n(0)∣H′∣n(0)⟩E_n^{(1)} = \langle n^{(0)} | H' | n^{(0)} \rangle First-order state correction:<br>∣n(1)⟩=∑m≠n⟨m(0)∣H′∣n(0)⟩En(0)−Em(0)∣m(0)⟩|n^{(1)}\rangle = \sum_{m\neq n} \frac{\langle m^{(0)}|H'|n^{(0)}\rangle}{E_n^{(0)} - E_m^{(0)}}|m^{(0)}\rangle<br>Second-order energy: En(2)=∑m≠n∣⟨m∣H′∣n⟩∣2En(0)−Em(0)E_n^{(2)} = \sum_{m\neq n} \frac{|\langle m|H'|n\rangle|^2}{E_n^{(0)}-E_m^{(0)}}.

Variational Principle and WKB

Variational principle: For any trial state ∣ψ⟩|\psi\rangle, ⟨H⟩≥Eground\langle H\rangle \geq E_{ground}. Used to estimate ground state energies.

WKB approximation (semiclassical): valid when de Broglie wavelength varies slowly. Tunnel probability:<br>T≈exp⁡(−2ℏ∫ab2m(V(x)−E) dx)T \approx \exp\left(-\frac{2}{\hbar}\int_a^b \sqrt{2m(V(x)-E)}\, dx\right)

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Degenerate Perturbation Theory

When H0H_0 has degenerate energy levels, use the 'good' linear combinations that diagonalise H′H' within the degenerate subspace. Ordinary first-order theory breaks down for degeneracy.

First-order perturbation theory gives En(1)=0E_n^{(1)} = 0 when H′H' is:

The variational method provides an upper bound on the:

Sketch how tunnelling current in a scanning tunnelling microscope (STM) depends on the tip-sample distance, using the WKB formula.