The process of stimulated Raman scattering (SRS) allows to convert laser em
ission wavelengths of materials providing suitable molecular or lattice mod
es which Contribute to the third order nonlinear optical susceptibility. SR
S of known materials can produce Stokes or anti-Stokes shifts in the range
of about 100 to 3100 cm(-1). Renewed interest in this field emerged because
of the discovery of SRS in crystals and glasses that contain molecular uni
ts exhibiting Raman active modes. Particularly, organic nonlinear,optical m
aterials used so far for frequency doubling and third harmonic generation s
eem to have a I great potential for SRS applications. SRS laser systems are
of interest in various fields including remote sensing of the atmosphere,
which requires high peak-power laser pulses at wavelengths that are difficu
lt to reach by current all-solid-state lasers. For SRS there is no need to
have acentric materials, therefore, many of the organic crystals and polyme
rs showing pronounced chi ((3)) properties may be reconsidered for a thus f
ar unexplored direction in the manufacturing of all-solid-state laser frequ
ency converters.