Bragg grating structure
View Patent ↗A Bragg grating has a local reflection strength which varies with position along the length of the grating so as to generate a non-uniform wavelength reflection spectrum, enabling compensation for a non-uniform gain profile of the gain section of a tunable laser. In another aspect, a Bragg comb grating is modulated by an envelope function which can also compensate for a non-uniform gain profile. The comb grating may be a phase change grating, with the envelope function shape being controlled by the length between phase changes and/or size of the phase changes.
1. A tunable laser comprising a gain section bounded at each end by a reflector, the gain section having a non-uniform wavelength gain profile, wherein at least one of the reflectors is a Bragg grating adapted to produce a reflection spectrum comprising a comb of reflective peaks at discrete wavelengths, the peaks having reflection amplitudes modulated by an envelope function which extends between two wavelength extremities, the grating comprising a plurality of periodic grating sections, each having a different pitch, wherein the relative reflective strength of the grating sections is varied with position along the length of the grating to control the envelope function, the reflection spectrum of the grating having an amplitude envelope function adapted to vary with wavelength between the two wavelength extremities in an opposite fashion to the gain profile so as to compensate at least partially for the non-uniform gain profile.
2. A method of increasing the usable tuning range of a tunable laser having a gain section bounded at each end by a reflector, at least one of the reflectors being a Bragg reflector adapted to produce a reflection spectrum comprising a comb of reflective peaks at discrete wavelengths, the peaks having reflection amplitudes modulated by an envelope function which extends between two wavelength extremities, the grating comprising a plurality of periodic grating sections, each having a different pitch, wherein the relative reflective strength of the grating sections is varied with position along the length of the grating to control the envelope function, the gain section having a non-uniform wavelength gain profile, the method comprising at least partially compensating for the non-uniform gain profile by adapting the Bragg reflector so that its wavelength reflection spectrum has an amplitude envelope function which varies with wavelength between the two wavelength extremities in an opposite fashion to the non-uniform gain profile.