“…The small wavelength variation of $4 nm in the emission wavelengths of these lasers are due to lateral wafer inhomogeneities, which can include variation of strain state, composition, layer thickness, and carrier density. [15][16][17][18][19] As the excitation power density increased, the spectral linewidth narrowed significantly and reached FWHM values of 1.4-2.3 nm at respective maximum excitation power density, which indicated stimulated emission. 2,3 The laser thresholds were estimated to be 280, 250, and 290 kW/cm 2 for the 239-nm, 242-nm, and 243-nm lasers, respectively.…”