The dependence of waveguide design parameters on the performance of a GaAs=AlGaAs quantum cascade laser emitting at 77 m is theoretically evaluated. We propose a new waveguiding scheme for modal conÿnement at such long wavelengths. An artiÿcially tailored index layer and a plasmon enhanced layer act
Design optimization of quantum cascade laser structures at λ ∼ 11-12 µm
✍ Scribed by Ko, Yeong Hwan ;Yu, Jae Su
- Publisher
- John Wiley and Sons
- Year
- 2010
- Tongue
- English
- Weight
- 446 KB
- Volume
- 207
- Category
- Article
- ISSN
- 0031-8965
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
By a simulation optimization technique, we design In~0.53~Ga~0.47~As/In~0.52~Al~0.48~As quantum cascade laser (QCL) structures, based on a four‐quantum well (QW) active region. The design of QCL structures is performed by maximizing an objective function, i.e., $z_{{\rm UL}}^2 (1 - \tau _{\rm L} /\tau _{{\rm UL}} )\tau _{\rm U}$, related to the optical gain, including dipole matrix element ($z_{{\rm UL}}$) and population inversion between subbands. For a specific lasing wavelength, each barrier/well layer in the active region can be optimized to maximize the objective function, which results from the increase in the dipole matrix element and the reduction in the lifetime ratio of $\tau _{\rm L} /\tau _{{\rm UL}}$, by an iterative procedure. The optimized QCL structures are obtained for the target wavelengths from 11 to 12 µm by a step of 0.5 µm. For a QCL structure operating at λ = 11.98, it exhibits the maximized objection function of 6.30 ps‐nm^2^ with a large dipole matrix element under an electric field of 45 kV/cm. The influence of the percent variation of thickness in In~0.53~Ga~0.47~As and In~0.52~Al~0.48~As layers by the change in growth rate on the lasing wavelength and objective function is also investigated.
📜 SIMILAR VOLUMES
## Abstract Optical waveguide structures of InP‐based quantum cascade lasers (QCLs) are theoretically analyzed and designed using the finite element method. The optical confinement factor (__Γ__) and absorption coefficient (__α__) of the waveguide structures for __λ__ ∼ 4.6, 6, 8.8, and 9.5 µm QCLs