Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 2 - Simple Design Consideration of Vertical Cavity Surface Emitting Lasers

CHAPTER 2

Simple Design Consideration of Vertical Cavity Surface Emitting Lasers

In this chapter, the simple design methodology of vertical cavity surface emitting lasers (VCSELs) under the criteria of minimum threshold current, maximum electronic conversion (current : gain) ratio as well as maximum wallplug (electrical-to-optical) efficiency are described. The corresponding design equations for VCSELs with uniform and periodic gain structures are derived for the investigation. Hence, the detailed structure of lasers can be determined for optimal performance at and above threshold operation.

2.1 INTRODUCTION

Vertical cavity surface emitting lasers (VCSELs) have optical cavities orthogonal to those of conventional facet emitting lasers [1 3]. This simple arrangement in the orientation of cavity significantly improves the output performance and fabrication flexibility of semiconductor lasers [4]. The main advantages of VCSELs over conventional facet emitting lasers are

  • VCSELs emit optical beams with low divergence and a circular symmetric profile because of their wide emission surface. As a result, the coupling efficiency to optical fiber and other optical components can be improved effectively [5].

  • VCSELs exhibit extremely high relaxation oscillation frequency (>70 GHz) [6] because of their short photon lifetimes. Consequently, high modulation bandwidth can be achieved.

  • VCSELs facilitate wafer-scale fabrication and testing by allowing fully monolithic processes because of their vertical orientation. Therefore, the production cost and procedures for quality inspection can be reduced enormously [4,5].

Hence, VCSELs are considered as the key components in optical fiber communications, optical interconnection systems, and optical parallel processing systems.

Because of the difference between VCSELs and conventional facet emitting lasers in cavity orientation, the design consideration of facet emitting lasers may not be applied to the analysis of VCSELs. For example, the requirement of high longitudinal side-mode suppression is the major concern in the design of facet emitting lasers [7,8] but is neglected in VCSELs [4] because of the latter s extremely short cavity length. Furthermore, in facet emitting lasers, maximum wallplug (electrical-to-optical) efficiency is achieved by enhancing the transverse confinement factor (i.e., overlap between transverse field profile and optical gain) [7,8], but that is realized in VCSELs with an optimal longitudinal confinement factor (i.e., overlap between longitudinal standing wave and optical gain) [9,10]. In addition, diffraction loss, self-heating, and high reflectivity (>0.95), which are the unique characteristics of VCSELs [11 16], need to be taken into consideration in the design of high-performance VCSELs. By contrast, diffraction loss and self-heating are usually ignored in the design of facet emitting lasers [7,8]. So, it can be concluded that the design criteria of VCSELs are quite different from those of facet emitting lasers.

In this chapter, the design methodology of VCSELs for optimal electrical and optical performance is discussed. The design equations for VCSELs with uniform and periodic gain structure are derived to optimize the corresponding threshold current density and differential quantum efficiency. In addition, the use of the quantum-well (QWs) active layer to enhance the steady-state performance of VCSELs is studied. It is shown that the design criteria of VCSELs are different from those of facet emitting lasers such as the requirement of extremely high reflectivity. Hence, equations for analysis and design of high-reflectivity multilayered mirrors are also given. Furthermore, the abovementioned threshold characteristics of VCSELs are optimized by analyzing the corresponding wallplug eficiency with the parasitic resistance and leakage current factored into the analysis.

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