Abstract
The propagation through a Raman medium of a pulse with several frequency components ωn= ω0 + nωR , where ω0 is the initial laser frequency and ωR is the frequency of the Raman transition of the molecules in the medium, has recently been treated1 by a detailed theory that includes the full quantum mechanical molecular dynamics of the (assumed two-state) molecules in the medium.
© 1987 Optical Society of America
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