Travelling wave model of a multimode Fabry-Perot laser in free running and external cavity configurations

• Published in: IEEE journal of quantum electronics Vol. 32; no. 3; pp. 553 - 566
• Main Authors: Homar, M., Moloney, J.V., San Miguel, M.
• Format: Journal Article
• Language: English
• Published: New York, NY IEEE 01.03.1996; Institute of Electrical and Electronics Engineers
• Subjects: Doped-insulator lasers and other solid state lasers; Equations; Exact sciences and technology; Fabry-Perot; Fundamental areas of phenomenology (including applications); General laser theory; Laser feedback; Laser modes; Lasers; Optical materials; Optics; Physics; Polarization; Reflectivity; Semiconductor device noise; Semiconductor lasers; laser diodes; Semiconductor materials; Spontaneous emission; Multimode laser; Travelling waves; Semiconductor lasers; Solid state lasers; Theoretical study; Mathematical models; Fabry Perot resonator; External cavity; Free running laser
• ISSN: 0018-9197; 1558-1713
• DOI: 10.1109/3.485410

We report the results of a numerical study of multimode behaviour of a Fabry-Perot laser. The model is based on travelling-wave equations for the slowly varying amplitudes of the counterpropagating waves in the cavity, coupled to equations for spatially dependent population inversion and polarization of a two-level active medium. Variations in the material variables on the scale of a wavelength are taken into account by means of an expansion in a Fourier series. Results are given for typical semiconductor laser parameters. Spatially distributed spontaneous emission noise and carrier diffusion are taken into account. The competing roles of spatial hole burning (SHE), spontaneous emission noise, and carrier diffusion in determining multimode behaviour are elucidated; with no carrier diffusion, spontaneous emission noise excites a large number of modes close to threshold, while SHE leads to a fixed number of significant lasing modes well above threshold. Carrier diffusion washes out the gratings in the material variables, and the resulting strengthening of the inter-mode coupling (cross-saturation) restores dominant single-mode emission well above threshold. We have also studied the effects of optical feedback and opportunities for mode selection with short external cavities; for an external cavity much shorter than the laser cavity length and a small field amplitude reflectivity coefficient, a single mode can be selected. For a large reflectivity coefficient, two groups of intracavity modes separated by the external cavity mode interspacing are selected. For an external cavity with a round trip time half that of the laser cavity, the laser can be forced with modest feedback to operate on two modes that are both quasiresonant with the external cavity. Mode selection is not found, even for weak feedback, when the external mode spacing is about 90% of the laser mode spacing.