Selection Rules:
Selection Rules Each of the spectroscopies have associated selection rules. Selection rules originate from the quantum mechanical description of electromagnetic radiation interaction with matter. Use time-dependent perturbation theory to derive probability of excitation between two states. Consider a two-level system Molecular Spectroscopy CEM 484 2
General Properties Wavefunctions are Normalized Orthonormal Wavefunctions are eigenstates of a specific operator Molecular Spectroscopy CEM 484 3
Iclicker: Eigenstates Which of the following functions are eigenstates of the hamiltonian, Ĥ o = d/dx A - Ψ = x B - Ψ = x 2 C - Ψ = e x D - Ψ = e x^2 Molecular Spectroscopy CEM 484 4
Perturbative Hamiltonian Apply perturbation theory H = H o + H 1 Ĥ o is independent of time. Separated time and spatial parts ψ 1 (r,t) = ψ 1 (r) ψ 1 (t) Ĥ o ψ 1 = E 1 ψ 1 = ihbar d ψ 1 /dt Interaction with radiation is represented by perturbative component Ĥ 1 depends on time and radiation. Ĥ 1 = - m E = - m E 0 cos2 pn t Molecular Spectroscopy CEM 484 5
Total wavefunction Total wavefunction a linear combination of eigenstates ψ = (a 1 ψ 1 + a 2 ψ 2 ) Probability of finding system in state 2 at time t is given by * (t)a 2 (t) P 1→2 = a 2 Finally get to P 1→2 = |< m > 12 | d (E 2 -E 1 -h n ) Molecular Spectroscopy CEM 484 6
Excitation Probability (1) Evaluate time-dependent Schrodinger equation to determine excitation probability Molecular Spectroscopy CEM 484 7
Excitation Probability (2) Evaluate time-dependent Schrodinger equation to determine excitation probability Molecular Spectroscopy CEM 484 8
Excitation Probability (3) Evaluate time-dependent Schrodinger equation to determine excitation probability Molecular Spectroscopy CEM 484 9
Rotational Selection Rules (1) Selection rule comes from < m > 12 = ∫ ψ 2 * m z ψ 1 dr Molecular Spectroscopy CEM 484 10
Rotational Selection Rules (2) Selection rule comes from Summary Molecular Spectroscopy CEM 484 11
Harmonic Oscillator Selection Rules (1) Selection rule comes from < m > 12 = ∫ ψ 2 * m z ψ 1 dr m z (x) = m 0 + (d m /dx) 0 q + … Molecular Spectroscopy CEM 484 12
Harmonic Oscillator Selection Rules (2) Selection rule comes from < m > 12 = ∫ ψ 2 * m z ψ 1 dr m z (x) = m 0 + (d m /dx) 0 q + … Summary Molecular Spectroscopy CEM 484 13
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