Vernier effect DBR lasers incorporating integrated tuning elements
Disclosed is a Vernier effect DBR laser that has uniform laser injection current pumping along the length of the laser. The laser can include one or more tuning elements, separate from the laser injection element, and these tuning elements can be used to control the temperature or modal refractive index of one or more sections of the laser. The refractive indices of each diffraction grating can be directly controlled by temperature changes, electro optic effects, or other means through the one or more tuning elements. With direct control of the temperature and/or refractive indices of the diffraction gratings, the uniformly pumped Vernier effect DBR laser can be capable of a wider tuning range. Additionally, uniform pumping of the laser through a single electrode can reduce or eliminate interfacial reflections caused by, for example, gaps between metal contacts atop the laser ridge, which can minimize multi-mode operation and mode hopping.
1. A semiconductor laser comprising:
a first grating section;
a second grating section;
a first set of diffraction gratings included in the first grating section, the first set of diffraction gratings comprising multiple first groups of grating elements;
a second set of diffraction gratings included in the second grating section, the second set of diffraction grating comprising multiple second groups of grating elements;
one or more tuning sections;
an optical gain region;
a first electrode disposed on the optical gain region and at least one of the first or second grating sections, the first electrode coupled to a first source configured to provide a first driving current to the optical gain region; and
one or more second electrodes, each second electrode disposed on at least one of the one or more tuning sections, wherein the one or more second electrodes are disposed in a section different from the first and second grating sections and coupled to a second source separate from the first source and configured to provide a second driving current to the one or more tuning sections to control properties of the at least one of the first or second grating sections,
wherein:
each group of the multiple first groups of grating elements is separated by a first spacing;
each group of the multiple second groups of grating elements is separated by a second spacing different than the first spacing;
the semiconductor laser includes a reflection spectrum comprising a plurality of peaks with a wavelength spacing;
a periodicity of each of the grating elements of the multiple first groups of grating elements are linearly varied; and
the first electrode is independently controllable from the one or more second electrodes such that a change of one is independent from a change of the other.
2. The laser of claim 1 , further comprising:
a trench located at least partially between the first electrode and at least one of the one or more second electrodes.
3. The laser of claim 2 , wherein the trench is associated with at least one of the one or more second electrodes, and an injection of a current into the at least one of the one or more second electrodes generates heat.
4. The laser of claim 2 , further comprising:
a second trench different from the trench and associated with a different one of the first or second grating sections.
5. The laser of claim 1 , wherein the wavelength spacing of the first grating section is different from the wavelength spacing of the second grating section.
6. The laser of claim 5 , further comprising:
a first region located between the first grating section and the second grating section, wherein the first region excludes diffraction gratings.
7. The laser of claim 6 , wherein the first region includes a phase section, the laser further comprising:
a third electrode disposed proximate to the phase section.
8. The laser of claim 5 , wherein an area of the first grating section is different from an area of the second grating section.
9. The laser of claim 1 , further comprising:
at least one of a sampled grating (SG) Distributed Bragg Reflector (DBR), phase-reversal grating DBR, superstructure grating (SSG) DBR, and binary superposition grating (BSG) DBR.
10. The laser of claim 1 , wherein the laser includes an optical cavity reflectance spectrum comprising a single peak, within an active region gain spectrum of the laser, formed by reflectance peaks from the first and second grating sections that overlap at least partially, wherein the plurality of output peaks excludes an interfacial reflectance.
11. The laser of claim 1 , wherein each of the one or more tuning sections is a heater or a phase section.
12. The laser of claim 1 , wherein a length of the first electrode is substantially equal to a length of the laser, wherein the length of the laser is along a direction of light propagation in the optical gain region.
13. The laser of claim 1 , wherein the laser is included in a device, the device further comprises:
one or more electrical sources, each source coupled to one of the one or more second electrodes; and
a controller coupled to the one or more sources and configured to adjust the one or more sources based on at least one of a temperature of one of the first or second grating sections, a temperature of the active region, an emission wavelength, an output power, and a tuning range.
14. The laser of claim 1 , wherein the laser is capable of continuous tuning within a single channel, wherein the single channel corresponds to a range of wavelengths.
15. The semiconductor laser of claim 1 , wherein two or more grating sections are first portions of the optical gain region are located in first sections, and a second portion of the optical gain region are located in a second section, the first sections separate from the second section.
16. A method of driving a laser having a waveguide, a first tuning element, a second tuning element, and two or more grating sections, the method comprising:
applying a first waveform to a first electrode of the first tuning element to control a first reflectance spectrum, wherein the first electrode is disposed in a section different from the two or more grating sections and the first electrode is coupled to a first source configured to provide a first driving current to the first tuning element;
applying a second waveform to a second electrode of the second tuning element to control a second reflectance spectrum, wherein the second electrode is disposed in a section different from the two or more grating sections and coupled to a second source different from the first source and configured to provide a second driving current to the one or more tuning sections to control properties of the at least one of the one or more grating sections;
applying a third waveform to the waveguide to control a third reflectance spectrum, wherein the third reflectance spectrum includes a plurality of reflectance peaks located at locations where the first reflectance spectrum and the second reflectance spectrum overlap; and
modulating at least one of the first, second, and third waveforms to continuously tune the laser, wherein:
a first set of diffraction gratings included in a first grating section of the two or more grating sections, the first set of diffraction gratings comprising multiple first groups of grating elements;
a second set of diffraction gratings included in a second grating section of the two or more grating sections, the second set of diffraction gratins comprising multiple second groups of grating elements;
each group of the multiple first groups of grating elements is separated by a first spacing;
each group of the multiple second groups of grating elements is separated by a second spacing different than the first spacing; and
a periodicity of each of the grating elements of the multiple first groups of grating elements are linearly varied.
17. The method of claim 16 , wherein the third waveform excludes reflectance peaks due to optical reflections at an interface or a boundary between sections of the laser.
18. The method of claim 16 , wherein at least two of the first, second, and third waveforms are modulated simultaneously.
19. The method of claim 16 , wherein all of the first, second, and third waveforms are modulated to achieve continuous tuning.
20. The method of claim 16 , wherein applying the third waveform includes uniform distribution along a length of the laser.
21. The method of claim 16 , wherein the laser further comprises a third tuning element, the method further comprising:
applying a fourth waveform to the third tuning element to control an optical path length of a cavity of the laser.