“…The carrier-density-dependent internal loss can be presented as n int 0 int σ α α + = (28,29), where α 0 is the constant component (which can be caused by scattering at rough surfaces or absorption in the cladding layers), σ int is the effective cross section for internal absorption loss processes, n is the free-carrier density in the optical confinement layer (OCL), and the component n int σ is caused by free-carrier absorption in the OCL. In the presence of such a loss, the lasing condition is written as (17,28,29) , [1] where g max is the maximum value of the gain (30), f n is the confined-electron level occupancy in QDs, ( ) ( ) R L 1 ln 1 = β is the mirror loss, L is the cavity length, and R is the facet reflectivity.…”