Frankly, Stimulated Raman Spectrosocpy is not a useful spectroscopic tool. The line/vibration with the highest gain reaches threshold first, reduces the overall gain of other lines and so dominates the specta. So instead of seeing a spectral fingerprint of all lines and species present, the spectrum consists of a single line (or often other lines associated with Stokes and anti-Stokes features of the majority species). For example, suppose one wished to monitor impurities in ethanol with SRS. Generally what you would see is only the 2928 cm-1 feature associated with the majority species ethanol and no sign of impurities.
Consequently, spontaneous Raman scattering spectroscopy remains a popular tool yielding an easily obtained fingerprint of all vibrations/species present. Occasionally, some nonlinear approaches like CARS (Coherent Anti-Stokes Raman Spectrosocpy) are used in special cases (as for example, when background light levels are a problem, say in a flame).
The closest spectroscopy related to SRS is cw coherent Raman gain spectroscopy popularized by Owyoung in the 70's (see for example, http://ieeexplore.ieee.org/xpl/login.jsp?tp=&arnumber=1069760&url=http%3A%2F%2Fieeexplore.ieee.org%2Fiel5%2F3%2F22982%2F01069760.pdf%3Farnumber%3D1069760 ). It doesn't seem to be in use much nowadays, perhaps because of the need for several tunable lasers (too complex, expensive).