fig3 is a schematic diagram , similar to the type of diagram included in fig2 , showing the variation in grating pitch of an embodiment of a distributed bragg reflector grating according to the invention . in particular , the diagram shows the variation in grating pitch as a function of position along the grating . the entire grating includes eight chirped grating sections , each of which has a respective electrical contact ( electrode ) associated with it , indicated by the reference numerals 65 - 72 . the variation in grating pitch for a known monotonically chirped grating ( also comprising eight chirped grating sections of corresponding length ) is indicated , for comparison , by the dotted line . each of the chirped grating sections of the grating according to the invention is shown to have a greater range of grating pitches than a corresponding chirped grating section of a conventional grating with the same profile of median grating pitches . consequently , there are discontinuities in the range of grating pitches , such that adjacent chirped grating sections have a sub - range of grating pitches in common ( i . e . they have partially overlapping grating pitches ). this produces a “ slatted ” arrangement in the grating pitch profile , as illustrated in the figure . the chirped grating sections may be ordered such that their median grating pitches form a monotonic series and there are no spatial gaps ( i . e . regions of the dbr without written grating ) between physically adjacent chirped grating sections . fig4 shows , schematically , the effect of the application of a tuning current to one section of an embodiment of a dbr grating according to the invention . this embodiment is similar to that shown in fig3 , and enables a direct comparison with the known grating shown in fig2 . additionally , the grating sections and the grating pitch line have been labelled in the same way as in fig2 . as can be seen , the effect of the application of a tuning current to the grating section labelled 98 is similar to the effect produced in the known grating shown in fig2 , except that the reinforced ( enhanced ) reflection peak 103 that is produced contains a broader range of wavelengths than does the corresponding reflection peak produced by the known grating . as explained above , this is due to the greater range of grating pitches provided by each grating section of this embodiment of the grating according to the invention , than provided by each grating section of the known grating . the consequent reflection trough 104 is also broader than that shown in fig2 , for the same reason . as explained above , a broader reinforced peak ( i . e . containing a broader range of wavelengths ) can , for example , provide advantages for a tuneable laser containing such a bragg reflector grating according to the invention . in particular , it can provide the advantage of allowing a greater tuning range within the reinforced peak , for a reflection peak produced by another grating at the opposite end of the laser . consequently , the provision of chirped grating sections with broader grating pitch ranges can provide improved wavelength tuning control . it can also permit greater manufacturing tolerances , because a greater degree of variability in construction can be accommodated . fig5 shows , schematically , the variation in grating pitch with position along the bragg grating reflector , of another embodiment of a bragg reflector grating according to the invention . in this embodiment , five chirped grating sections ( out of a total of eight chirped grating sections ) having grating pitch ranges approximately in the middle of the entire range of grating pitches for the entire dbr grating , have partially overlapping grating pitch ranges . as explained above , this can be advantageous because the gain spectrum of the gain section of a tuneable laser often has a maximum peak towards the middle of the tuning range , which can lead to a non - uniformity in the laser &# 39 ; s side - mode suppression ratio ( smsr ). by producing a dbr grating in which sections corresponding approximately with the middle of the pitch range include pitch range overlaps ( while those at the ends of the range do not , or at least have smaller overlaps ), the reinforced reflection peaks produced by tuning will generally be stronger ( of greater power ) at the ends of the wavelength range than in the middle . in this way the present invention can be used to profile the strength of the dbr grating , and / or peaks formed by reinforcement of the reflections of different chirped grating sections by tuning , as a function of position . this can serve to improve the uniformity of the smsr across the tuning range , and thus can increase performance and / or manufacturing yield . it can additionally or alternatively be desirable to provide overlapping pitch ranges at one end of the dbr grating ( and not at the other end ). fig6 shows , schematically , the variation in grating pitch with position along the bragg grating reflector , of a further embodiment of a reflector according to the invention . in this embodiment , the discontinuities in the grating pitch variation between the chirped grating sections comprise gaps , or absences , in the grating pitch range , such that the grating pitch variation has a stepped profile . this illustrates the design flexibility enabled by the present invention , which allows bragg reflector gratings to be designed to meet any of a variety of different requirements . in particular , it enables the provision of a variety of tuneable lasers , meeting any of a variety of requirements . with the present invention , due to the discontinuity ( or discontinuities ), it is possible to control the local pitch gradient and the median pitch of chirped grating sections independently of adjacent sections . it will of course be understood that many variations may be made to the above - described embodiments without departing from the scope of the present invention .