“…in the estimation of the Raman gain coefficient, it is more appropriate to use a level slightly below that of the laser pump intensity when the first Stokes lasing becomes perceptible. Examples of single-and manyphonon Stokes and anti-Stokes generation spectra of two widely used inorganic laser host crystals GdVO 4 [354,355] and α-KY(WO 4 ) 2 [337], two organic crystals with predominantly ionic [C(NH 2 ) 3 ]Zr{N(CH 2 COO) 3 ] 2 · H 2 O (GuZN-III) [379]) and van der Waals C 12 H 22 O 11 (α-dglucopyranosido-β-d-fructofuranoside (sucrose), a crystalline food sugar) [443]) structural units, three fluorides with the fluorite structure (CaF 2 [742], SrF 2 [801], and BaF 2 ), as well as two novel promising SRS-active crystals with high Raman gain coefficients (SC-CVD diamond [720] and Na 3 Li(SeO 4 ) 3 · 6H 2 O [734]) and are given in Figs. 24-30. As can be seen from these spectra the organic crystals show significantly larger Stokes and anti-Stokes shifts.…”