“…With respect to the latter, each SDL gain structure has an optimum temperature at which the gain and the resonances overlap such that the effective gain is optimised, beyond which thermal rollover will eventually shut off the laser. However, while this overlap can be partly accounted for by designing in an appropriate offset for the cold laser, 37 for example, the room temperature RPG wavelength may be fi xed at a longer wavelength than the peak of the quantum well gain (which has higher d λ /d T ), thermal escape of the carriers from the quantum wells limits high temperature operation. The pump induced temperature increase, therefore, ultimately limits the maximum output power of an SDL.…”