Phase-control in an external-cavity tuneable laser
View Patent ↗A single-mode external-cavity tuneable laser includes a gain medium, a tuneable element and a channel allocation grid element. The channel allocation grid element is preferably an FP etalon which is structured and configured to define a plurality of equally spaced transmission peaks corresponding to the ITU channel grid, e.g., 200, 100, 50 or 25 GHz. The tuneable element, preferably a tuneable mirror, serves as the coarse tuning element that discriminates between the peaks of the grid etalon. The tuneable laser of the invention has a relatively short cavity length of not more than 15 mm, preferably not larger than 12 mm. It has been found that the FP etalon introduces a phase non-linearity in the external cavity, which induces a compression of the cavity modes, i.e., a reduction in the cavity mode spacing, in correspondence to the etalon transmission peaks. Mode compression increases with the decrease of the FWHM bandwidth of the grid FP etalon, hereafter referred to as (FWHM) FP . (FWHM) FP should be about 2 GHz to about 8 GHz. Preferably, (FWHM) FP is approximately 3 to 6 GHz.
1. A tunable laser system configured to emit output radiation on a single longitudinal mode at a laser emission frequency, comprising:
an external cavity having a physical length and a plurality of cavity modes;
a gain medium to emit an optical beam into the external cavity;
a channel allocation grid element being arranged in the external cavity to define a plurality of periodic pass bands substantially aligned with corresponding channels of a selected wavelength grid, each of the pass bands having a bandwidth at full-width half maximum (FWHM); and
a tunable element arranged in the external cavity to tuneably select one of the pass bands so as to select a channel to which to tune the optical beam,
wherein said physical length of the external cavity is not larger than 15 mm and the bandwidth FWHM of the channel allocation grid element is 2 to 8 GHz.
2. The laser system according to claim 1 , wherein the bandwidth of the channel allocation grid element at FWHM is 3 to 6 GHz.
3. The laser system according to claim 1 , wherein the physical length is not larger than 12 mm.
4. The laser system according to claim 1 , wherein the laser emission frequency is selected on a single cavity mode within a given frequency accuracy which is not smaller than 0.5 GHz and the bandwidth of the channel allocation grid element at FWHM is selected so that the minimum distance between two adjacent cavity modes of the external cavity within the pass bands of the channel allocation grid element is not larger than twice the frequency accuracy.
5. The laser system according to claim 1 , wherein the selected wavelength grid has a channel spacing of 25 to 200 GHz.
6. The laser system according to claim 1 , wherein the selected wavelength grid has a channel spacing of 25 or 50 GHz.
7. The laser system according to claim 1 , wherein the channel allocation grid element comprises a Fabry-Perot etalon.
8. The laser system according to claim 7 , wherein the Fabry-Perot etalon is placed at an inclination angle of 0.4° to 0.8° to the perpendicular of the optical beam.
9. The laser system according to claim 7 , wherein the Fabry-Perot etalon is placed at an inclination angle of 0.5° to the perpendicular of the optical beam.
10. The laser system according to claim 1 , wherein the tunable element has a bandwidth at FWHM of 50 to 250 GHz.
11. The laser system according to claim 10 , wherein the tunable element has a bandwidth at FWHM of 50 to 100 GHz.
12. The laser system according to claim 1 , wherein the tunable element comprises a tunable mirror placed at one end of the external cavity.
13. The laser system according to claim 12 , wherein the tunable mirror is an electro-optical element that comprises a waveguide formed onto a substrate and a diffraction grating formed onto the waveguide.
14. The laser system according to claim 13 , wherein the tunable mirror further comprises a cladding layer that fills at least the interstices of the diffraction grating, said cladding layer comprising a liquid crystal material.
15. The laser system according to claim 1 , wherein the gain medium is a semiconductor laser diode.
16. The laser system according to claim 1 , wherein the laser emission frequency is selected on a single transversal cavity mode.
17. A method for controlling a laser emission frequency of a tunable laser system having an external cavity defining a plurality of cavity modes spaced from each other by (FSR) cavity , wherein the physical length of the external cavity is not larger than 15 mm, the laser emission frequency being selected on a single longitudinal cavity mode, comprising the steps of:
tuning an optical beam emitted from a gain medium to a corresponding centre frequency of a pass band selected from a plurality of periodic pass bands substantially aligned with corresponding channels of a selected wavelength grid element; and
selecting the bandwidth at FWHM of the selected pass band so that
2 GHz≦FWHM≦8 GHz, and
selecting the (FSR) cavity to be larger than about 8 GHz.
18. The method according to claim 17 , wherein the bandwidth at FWHM of the selected pass band is 3 to 6 GHz.
19. The method according to claim 17 , wherein the channels of the selected wavelength grid element have a channel spacing of 25 to 100 GHz.
20. The method according to claim 19 , wherein the bandwidth at FWHM of the selected pass band and s min satisfy the following relationship:
FWHM=α+β·s min
where α is −0.8 to −2.7 GHz and β is 1.2 to 2.6.
21. The method according to claim 17 , further comprising the step of aligning the laser emission frequency with the selected pass band by adjusting the injection current of the gain medium so as to maximise the laser output power.
22. A method for controlling a laser emission frequency of a tunable laser system having an external cavity defining a plurality of cavity modes spaced from each other by (FSR) cavity , wherein the physical length of the external cavity is not larger than 15 mm, the laser emission frequency being selected on a single longitudinal cavity mode within a given frequency accuracy, comprising the steps of:
tuning an optical beam emitted from a gain medium to a corresponding centre frequency of a pass band selected from a plurality of pass bands substantially aligned with corresponding channels of a selected wavelength grid element;
selecting the (FSR) cavity , to be larger than about 8 GHz; and
selecting the bandwidth at FWHM of the selected pass band to be comprised between about 2 GHz and about 8 GHz so as to introduce cavity mode compression in correspondence to the selected pass band and so as to cause the minimum distance between two adjacent cavity modes of the external cavity within the pass band, s min , to be not larger than twice the frequency accuracy.
23. The method according to claim 22 , wherein the frequency accuracy is not smaller than 0.5 GHz.