“…Measurements of natural linewidth for high power lasers: GaInAs/GaInAsP (SCH), (QW), (DFB LDs) lasers [1], gain-guided V-groove laser and oxide stripe laser [2], DFB Lasers [3][4][5], VCSEL laser [6], microcavity laser [7] and Fabry-Perot lasers [8][9][10] have shown various functional deviations from Schawlow-Townes formula [11] for natural linewidth for one mode =S 0 ·(1/ P ), (1) where S 0 =const, P is output power. Additional account of amplitude perturbations in semiconductor lasers [12] yielded the same modified formula (1) in which S 0 was changed to account for amplitude fluctuations. Various mechanisms, explaining occurrence of the contribution independent of output power at linewidth have been offered in the papers [9,13,14].…”