Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 4.5 - Polarozation Noise in VCSELs

4.5 POLAROZATION NOISE IN VCSELs

Polarization noise is presented in all semiconductor lasers but is exceptionally strong in VCSELs. This is because spontaneous emission noise, which is the driving force of the polarization noise, is relatively strong in VCSELs because of the enhancement of the spontaneous emission factor by the small cavity size. In addition, the deterministic forces of the polarizations (i.e., intrinsic optical anisotropies) are relatively small (i.e., compared with facet emitting lasers), due to the cylindrical symmetry of the corresponding waveguide geometry. Hence, the combination of strong stochastic noise and weak restoring force creates relatively large polarization fluctuation. In the practical applications of VCSELs, it is necessary to understand the corresponding mechanisms of polarization fluctuation in order to avoid unnecessary generation of intensity noise. In this section, the influence of the initial conditions and Langevin noise sources on the time evolution of the two orthogonal polarizations is studied. Furthermore, it can be shown that the polarization characteristics of VCSELs such as optical spectra can be utilized to extract the nonlinear parameters (i.e., gain anisotropy and birefringence) of the modified four-level model.

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