Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 7 - Direct Modulation of Vertical Cavity Surface Emitting Lasers

CHAPTER 7

Direct Modulation of Vertical Cavity Surface Emitting Lasers

Amplitude modulation response and second-harmonic distortion of VCSELs are derived analytically from a simple rate equation model. The transient response of multimode VCSELs is discussed and analyzed. In addition, the large-signal transient response of VCSELs such as gain switching is investigated. Comprehensive time-domain models of VCSELs including quasi-3D distribution of optical fields are also described. Finally, the effect of the hot carrier on the dynamic response of VCSELs is studied.

7.1 INTRODUCTION

Vertical cavity surface emitting lasers (VCSELs) are considered the key components in future high-speed optical fiber communication systems because of their potential capability for stable single-longitudinal-mode operation, extremely high intrinsic relaxation oscillation frequency, ultra-low-threshold current, and efficient coupling into optical fibers. The extremely high intrinsic relaxation oscillation frequency (ROF) of VCSELs is the result of high photon density inside the small laser cavity as the ROF is proportional to the square root of the photon density. It is demonstrated that the ROF of VCSELs can be as high as 71 GHz [1], but the maximum modulation bandwidth is limited to 16 GHz [2]. Because of the limitation of the modulation bandwidth, the transmission experiments (i.e., using 0.98-μm InGaAs/GaAs QWs proton-implanted/oxide-confined VCSELs) show that the maximum data rate has been restricted to 10 Gbits/s [3] and 12.5 Gbits/s [4] in a graded-index multimode fiber link 0.5 km long and in a standard single-mode fiber link 1.6 km long, respectively, with a minimum bit error rate of 10-11. Therefore, in order to increase the transmission rate of optical fiber communication systems, obstacles that can occur in the modulation bandwidth of VCSELs have to be minimized.

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