phy-4600/lecture_notes/3-18/overview

44 lines
1.2 KiB
Plaintext
Raw Permalink Blame History

This file contains ambiguous Unicode characters

This file contains Unicode characters that might be confused with other characters. If you think that this is intentional, you can safely ignore this warning. Use the Escape button to reveal them.

Vibrations and rotations of a diatomic molecule
atoms vibrate about an equilibrium position r₀
⊙~~~~~~~~~⊙
|← r₀ →|
(pic MISSEd) potential, with taylor approximation
(pic MISSEd) A taylor series solution is appropriate to solve this diffEQ.
Experiments indicate vibration (E~visible light) has more energy than rotation (E~infrared), so vibrations happen much faster.
The Rotational eigen-value spectrum
L²,L̂𝓍,L̂𝓎,L̂𝓏 (Hermition operators)
Say
𝓏❙Ψ❭ = mₗħ❙Ψ❭
(pic) mₗ is bound by λ: m has value from -λ to λ
Introduced raising and lower operators
L̂± = L̂𝓍 ± ι𝓎 = (pic) proof = ±ħL±
𝓏(L̂ ± ❙λ,mₗ❭) => (pic) proof => L̂± ❙λ,mₗ❭ = ❙λ,mₗ±1❭
Very important point:
Let m=l be the maximum value of m
L̂₊❙λ,l❭ = 0 (required because wave function goes to 0 in a forbiddin region)
This is also true for L̂₋❙λ,l❭ with l the minimum value of m
(pic) L̂₋L̂₊❙λ,l❭ = ...
gives λ = l(l+1)
(pic) L̂₊L̂₋❙λ,l❭ = ...
gives λ = l(l+1)
These show that m = -l, -l+1, 0, l