Abstract
The third-order susceptibility is expressed as a summation of interfering resonant terms, each involving the phenomenological linewidth of the transition. Correlations of the finite line-width of the laser sources with |<i>X</i><sup>(3)</sup>|<sup>2</sup> (coherent anti-Stokes Raman spectroscopy) and –<i>X"</i> (stimulated Raman scattering) are performed and closed-form expressions for the theoretical profiles are obtained.
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