Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 4.4.3 - Stability Analysis of Polarizations in Isotropic Medium

4.4.3 Stability Analysis of Polarizations in Isotropic Medium

The stability of the two orthogonal polarizations can be analyzed by the perturbation method. This can be done by assuming that the steady-state solutions of E±, N, and n have the form

where the subscript "s" stands for steady state, θa is an arbitrary phase that can be ignored, and θr is a relative phase. For the case of isotropy (i.e., γa = Ybf = 0), the two circularly polarized components degradation in amplitude and frequency can be deduced by setting the time derivative terms of (4.72)—(4.74) to zero, it can be shown that

where Ns → 1 and ns → 0 are assumed in the derivation of (4.81). Furthermore, the projections of the circular polarizations on the h and v directions are found to be

which are the orthogonal polarizations at an arbitrary value of θr. Therefore, it is shown that in a steady-state condition, this solution is linearly stable for any finite value of parameters, but if τJ → 0 (implies E-2E+2 → ∞) it becomes marginally stable with respect to amplitude fluctuations. This means that the finite value of τJ stabilizes the linearly polarized emission and destabilizes circularly polarized or elliptically polarized emission in an isotropic medium. In addition, the lasing frequency of the two orthogonal polarizations degenerates to zero as ns0 at steady state.

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