Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 4.6 - Summary

4.6 SUMMARY

In summary, this chapter investigates the intrinsic optical anisotropy of VCSELs. First, the formation of in-plane gain anisotropies in VCSELs is studied. It is shown that the in-plane gain anisotropy in VCSELs can be obtained from

  •  The saturation of optical gain arising from the high intensity of the two orthogonal polarizations
  •  The growth of QW epitaxial layers on the non (001) substrate
  •  The influence of birefringence on the modal gain of the two orthogonal polarizations

Hence, a simple rate-equation model (i.e., two-level model) is derived with in-plane gain anisotropies factored in to analyze the polarization dynamics of VCSELs. In the model, the amplitudes of the two orthogonal polarizations are coupled together through self- and cross-saturation coefficients of the nonlinear gain so that the conditions of polarization switching and polarization bistability of VCSELs can be investigated.

Second, the electrooptically induced birefringence due to the inevitable internal electric field inside the laser cavity of VCSELs is studied theoretically. A theoretical model based on the assumption of electrooptic birefringence is derived to analyze the frequency splitting between the two orthogonal polarizations. It is shown that the electrooptic birefringence is dominated mainly inside the multilayered mirrors of VCSELs. Using this model, the frequency splitting between the two orthogonal polarizations is calculated and compared with the experimental results. It is found that the frequency response of the two orthogonal polarizations is not only determined by the electrooptic birefringence but may also be affected by the gain anisotropy as well as other nonlinear effects due to the small cavity size of VCSELs.

Finally, a four-level model is described to analyze the polarization dynamics of VCSELs. This four-level model takes into account the spin sublevels of the conduction and valence bands of the QW materials. Therefore, the lasing field of different polarizations associated with the transition between different spin sublevels can be included in the calculation. It is assumed that the transition between the two orthogonal polarizations is coupled through the spin–flip relaxation process so that their phase information can be evaluated simultaneously. The model is utilized to study the stabilities of the two orthogonal polarizations under the influence of optical anisotropies. Furthermore, the four-level model is transformed into a one-dimensional polarization rate equation via spin elimination so that the noise properties of VCSELs at steady state are analyzed. Using this model, the laser parameters of VCSELs such as effective loss anisotropy and birefringence are evaluated from the measured polarization noise spectra of VCSELs.

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