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Integrated high-order surface diffraction gratings for diode lasers
- Source :
- Quantum Electronics. 45:1091-1097
- Publication Year :
- 2015
- Publisher :
- IOP Publishing, 2015.
-
Abstract
- High-order surface diffraction gratings acting as a distributed Bragg reflector (DBR) in mesa stripe semiconductor lasers (λ = 1030 nm) have been studied theoretically and experimentally. Higher order interfering radiation modes (IRMs), which propagate off the plane of the waveguide, have been shown to have a crucial effect on the reflection and transmission spectra of the DBR. The decrease in the reflectivity of the DBR in response to the increase in the diffraction efficiency of these modes may reach 80% and more. According to theoretical analysis results, the intensity of the higher order IRMs is determined by the geometry of the DBR groove profile. Experimental data demonstrate that the noncavity modes are responsible for parasitic light leakage losses in the laser cavity. It has been shown that, in the case of nonoptimal geometry of the grating groove profile, the overall external differential quantum efficiency of the parasitic laser emission may exceed 45%, which is more than half of the laser output power. The optimal geometry of the DBR groove profile is trapezoidal, with the smallest possible lower base. Experimental evidence has been presented that this geometry considerably reduces the power of the higher order IRMs and minimises the parasitic light leakage loss.
- Subjects :
- Physics
business.industry
Bragg's law
Statistical and Nonlinear Physics
Laser
Diffraction efficiency
Distributed Bragg reflector
Atomic and Molecular Physics, and Optics
Electronic, Optical and Magnetic Materials
law.invention
Semiconductor laser theory
Optics
law
Optical cavity
Optoelectronics
Electrical and Electronic Engineering
business
Waveguide
Diffraction grating
Subjects
Details
- ISSN :
- 14684799 and 10637818
- Volume :
- 45
- Database :
- OpenAIRE
- Journal :
- Quantum Electronics
- Accession number :
- edsair.doi...........35c1fe506332bf17fdc5f44afbcbbc8b