A full time-domain approach to spatio-temporal dynamics of semiconductor lasers. II. Spatio-temporal dynamics

被引:21
|
作者
Boehringer, Klaus
Hess, Ortwin [1 ]
机构
[1] Univ Surrey, Adv Technol Inst, Fac Engn & Phys Sci, Guildford GU2 7XH, Surrey, England
基金
英国工程与自然科学研究理事会;
关键词
Semiconductor lasers; Nonlinear optical pulse propagation; Numerical simulation of optoelectronic devices;
D O I
10.1016/j.pquantelec.2008.10.003
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
The spatio-temporal dynamics of novel semiconductor lasers is discussed on the basis of a space and momentum-dependent full time-domain approach. To this means the space-. time-, and momentum-dependent Full-Time Domain Maxwell Semiconductor Bloch equations, derived in(] discussed in our preceding paper I [K. Bohringer. O. Hess, A full time-domain approach to spatio-temporal dynamics of semiconductor lasers. I. Theoretical formulation], are solved by direct numerical integration. Focussing on the device physics of novel semiconductor lasers that profit, in particular, from recent advances in nanoscience and nanotechnology, we discuss the examples of photonic band edge surface emitting lasers (PBE-SEL) and semiconductor disc lasers (SDLs). It is demonstrated that photonic crystal effects can be obtained for finite crystal structures, and leading to a significant improvement in laser performance such as reduced lasing thresholds. In SDLs, a modern device concept designed to increase the power output of surface-emitters in combination with near-diffraction-limited beam quality, we explore the complex interplay between the intracavity optical fields and the quantum well gain material in SDL structures. Our simulations reveal the dynamical balance between carrier generation due to pumping into high energy states, momentum relaxation of carriers, and stimulated recombination from states near the band edge. Our full time-domain approach is shown to also be an excellent framework for the modelling of the interaction of high-intensity femtosecond and picosecond pulses with semiconductor nanostructures. It is demonstrated that group velocity dispersion. dynamical gain saturation and fast self-phase modulation (SPM) are the main causes for the induced changes and asymmetries in the amplified pulse shape and spectrum of an ultrashort high-intensity pulse. We attest that the time constants of the intraband scattering processes are critical to gain recovery. Moreover, we present new insight into the physics of nonlinear coherent pulse propagation phenomena in active (semiconductor) gain media. Our numerical full time-domain simulations are shown to generally agree well with analytical predictions, while in the case of optical pulses with large pulse areas or few-cycle Pulses they reveal the limits of analytic approaches. Finally. it is demonstrated that coherent ultrafast nonlinear propagation effects become less distinctive if we apply a realistic model of the quantum well semiconductor gain material, consider characteristic loss channels and take into account de-phasing processes and homogeneous broadening. (C) 2008 Elsevier Ltd. All rights reserved.
引用
收藏
页码:247 / 307
页数:61
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