Lecture 23
Stimulated Raman scattering, Stokes and anti-Stokes waves. Stimulated Brillouin scattering.
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Stimulated Raman scattering (SRS)
2 2
1 Stimulated Raman scattering (SRS)
We will see now how energy dissipation can lead to both field attenuation and field amplification.
3 3
Stimulated Raman scattering (SRS)
Molecule: vibrates at freq. Ω
Ω ω ω
ω±Ω
sidebands ±Ω
4 4
2 Stimulated Raman scattering (SRS)
Total field squared time averaged: 2 Back action [E1cos(ωt) +E2cos(ω–Ω)]
Ω
ω
ω–Ω time
This modulated intensity coherently excites the molecular oscillation at frequency ωL − ωS = Ω.
5 5
Stimulated Raman scattering (SRS)
Back action
ω q - normal coordinte
Dipole moment of a molecule: � = � �� ω–Ω key assumption of the theory: �� � = � + � �� Energy due the oscillating field E: 1 � = � �� 2 Two laser frequencies force molecule to vibrate at freq. Ω The applied optical field exerts a force �� 1 �� � = = � � �� 2 ��
6 6
3 Stimulated Raman scattering (SRS)