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 chirped Bragg grating having a local reflection strength which varies with position along the length of the grating so as to generate an overall reflection strength spectrum which is non-uniform with respect to wavelength between two wavelength extremities, and
comprising: a periodic pattern of marks and spaces whose period varies along the length of the grating; and one or more reduced reflective strength regions, each reduced reflective strength region formed by the base order periodic pattern of marks and spaces from which at least some of the marks are missing.
2. The grating of claim 1 , wherein the pattern in each of the reduced reflective strength regions is defined by the base order pattern modulated by a higher order envelope function that determines which marks are missing from the base order pattern.
3. The grating of claim 1 , wherein the reflection strength of the grating is higher for wavelengths at the extremities of the reflection strength spectrum than for wavelengths between the extremities.
4. The grating of claim 1 , wherein the reflection strength spectrum is asymmetric.
5. The grating of claim 1 , wherein the reflection strength of the grating increases from one wavelength extremity to the other wavelength extremity.
6. The grating of claim 5 , wherein the reflection strength of the grating varies substantially linearly with wavelength between the wavelength extremities.
7. 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 the Bragg grating of claim 1 , 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.
8. A tunable laser comprising a gain section bounded at each end by a reflector, at least one of the reflectors being the Bragg reflector of claim 1 , the reflection spectrum of the Bragg reflector having an amplitude envelope function adapted to vary with wavelength between the two wavelength extremities so as to compensate at least partially for wavelength-dependent optical cavity losses in the laser.
9. 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 the Bragg reflector of claim 1 , 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.
10. 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 is non-uniform between two wavelength extremities, the grating comprising a plurality of periodic grating sections separated by phase changes, the lengths of the grating sections being chosen so that the envelope function includes maxima at the two wavelength extremities.
11. The grating of claim 10 , wherein the envelope function has a dished shape.
12. The grating of claim 10 , wherein each phase change between sections is of π radians.
13. The grating of claim 10 , wherein the envelope function is asymmetric.
14. The grating of claim 13 , wherein the phase changes between grating sections are chosen to control the asymmetry of the envelope function.
15. A method of manufacturing a chirped Bragg grating having a non-uniform wavelength reflection spectrum, the method comprising varying the reflection strength along the length of the grating by forming a periodic pattern of marks and spaces whose period varies along the length of the grating; and one or more reduced reflective strength regions, each reduced reflective strength region formed by the base order periodic pattern of marks and spaces from which at least some of the marks are missing.