Analysis and Design of Vertical Cavity Surface Emitting Lasers

Chapter 4A - Appendix

4A APPENDIX

4A.1 Calculation of the Susceptibilities

The third-order susceptibilities associated with self-saturation coefficients in the frame of (,,) are given by [20]




There are three blocks, (i)–(iii), in (4A.l), each associated with the transition between the conduction band and the lowest, the second lowest, and the third lowest energy subbands in the valence band, respectively. A similar expression holds for , which can be obtained by replacing the directions of dipole transition matrix elements. Hence, the self-saturation coefficients in VCSELs can be obtained after appropriate coordinating transformations.

The third-order susceptibilities associated with cross-saturation coefficients are quite long and tedious. First consider(ωh, ωh, ωv), which yields a crosssaturation coefficient ζcvh of the VCSELs for the two orthogonal optical fields, one with frequency ωv in v mode and the other with frequency ωh in h-mode. This component consists of . The former is given by

where the term (i) associated with the transition between the lowest conduction subbands and the lowest valence subbands is given by the following expression:


This term is triply resonant when ωv =ωh = Ec(k) — Ev(k). The terms (ii) and (iii) are given by expressions similar to (4A.3) by replacing the summation indices. These three terms are related to the main peaks at ωv = ωh in the cross-saturation coefficients.

The term (iv) becomes triply resonant when ωv = Ec(k) — Ev(k) and ωh = Ec(k) — Ev(k), or vice versa. It is explicitly given by

Other cross-terms are given in a similar manner.

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