Abstract A tunable optical waveguide laser arrangement includes a solid optical waveguide capable of guiding light along an axis between axially spaced ends thereof and being at least in part of an excitable material that emits light in response to stimulation by light. Stimulating light is launched into the waveguide for axial propagation therein and attendant emission of light by the excitable material. Two end reflectors are situated in the waveguide, each at one of the axially spaced ends thereof and extending normal to the axis to delimit a laser cavity. Each of the reflectors is constituted by a Bragg grating consisting of a multitude of axially consecutive grating elements constituted by periodic refractive index perturbations with a given periodicity. The length of the cavity, the peak reflectivity of the Bragg gratings and the gain of the excitable material are so coordinated with one another as to enable lasing in only a single longitudinal mode. The length of that portion of the optical waveguide that incorporates the two Bragg gratings and an intervening region of the optical waveguide is uniformly controlledly varied with attendant continuous tuning of the laser output wavelength without longitudinal mode hopping.
A tunable optical waveguide laser arrangement comprising: a solid optical waveguide guiding light along an axis between axially spaced ends thereof and being located within a portion of an excitable material that emits coherent light in response to stimulation by pump light; means for launching said pump light into the waveguide for axial propagation therein and attendant emission of coherent light by the excitable material; two end reflectors each situated in the waveguide at one of the axially spaced ends thereof and extending normal to the axis to delimit a laser cavity, each of said reflectors being constituted by a Bragg grating consisting of a plurality of axially consecutive grating elements constituted by periodic refractive index perturbations with a given periodicity, the length of said cavity, the narrow peak reflectivity of said Bragg gratings and the frequency response of the gain of the excitable material being coordinated with one another such that lasing occurs only at a single longitudinal mode; and means for uniformly controlledly varying the length of that portion of said optical waveguide that incorporates the two Bragg gratings and an intervening region of said optical waveguide such that attendant continuous tuning of the laser output wavelength occurs without longitudinal mode hopping.
Claim 2
Dependent Claim
204 words
A tunable optical waveguide laser arrangement comprising: a solid optical waveguide guiding light along an axis between axially spaced ends thereof and being located within a portion of an excitable material that emits coherent light in response to stimulation by pump light; means for launching said pump light into the waveguide for axial propagation therein and attendant emission of coherent light by the excitable material; two end reflectors each situated in the waveguide at one of the axially spaced ends thereof and extending normal to the axis to delimit a laser cavity, each of said reflectors being constituted by a Bragg grating consisting of a plurality of axially consecutive grating elements constituted by periodic refractive index perturbations with a given periodicity, the length of said cavity, the narrow peak reflectivity of said Bragg gratings and the frequency response of the gain of the excitable material being coordinated with one another such that lasing occurs only at a single longitudinal mode; and means for uniformly controlledly varying the length of that portion of said optical waveguide that incorporates the two Bragg gratings and an intervening region of said optical waveguide such that attendant continuous tuning of the laser output wavelength occurs without longitudinal mode hopping.
Claim 3
Dependent Claim
50 words
The arrangement as defined in claim 1, wherein said material exhibits a gain that exceeds a lasing threshold only by an amount small enough for the product of gain and grating reflectivity to rise to a level at which lasing takes place only for said at most few longitudinal modes.
Claim 4
Dependent Claim
35 words
The arrangement as defined in claim 1, wherein the other of said reflectors is constituted by another grating substantially identical to said one Bragg grating and axially delimiting said laser cavity at said other end.