Volume 4, Issue 1-2 p. 1-3
Rapid Research Letter

Polarization of eigenmodes in laser diode waveguides on semipolar and nonpolar GaN

Jens Rass,

Corresponding Author

Institute of Solid State Physics, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany

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Tim Wernicke,

Ferdinand-Braun-Institut für Höchstfrequenztechnik, Gustav-Kirchhoff-Str. 4, 12489 Berlin, Germany

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Wolfgang G. Scheibenzuber,

Department of Physics, Regensburg University, 93040 Regensburg, Germany

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Ulrich T. Schwarz,

Department of Physics, Regensburg University, 93040 Regensburg, Germany

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Jan Kupec,

Integrated Systems Laboratory, ETH Zurich, Gloriastr. 35, 8092 Zurich, Switzerland

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Bernd Witzigmann,

Computational Electronics and Photonics Group, University of Kassel, Wilhelmshöher Allee 71, 34121 Kassel, Germany

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Patrick Vogt,

Institute of Solid State Physics, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany

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Sven Einfeldt,

Ferdinand-Braun-Institut für Höchstfrequenztechnik, Gustav-Kirchhoff-Str. 4, 12489 Berlin, Germany

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Markus Weyers,

Ferdinand-Braun-Institut für Höchstfrequenztechnik, Gustav-Kirchhoff-Str. 4, 12489 Berlin, Germany

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Michael Kneissl,

Institute of Solid State Physics, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany

Ferdinand-Braun-Institut für Höchstfrequenztechnik, Gustav-Kirchhoff-Str. 4, 12489 Berlin, Germany

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First published: 04 February 2010
Citations: 16

Abstract

Recent calculations of the eigenmodes in waveguides grown on semipolar GaN suggest that the optical polarization of the emitted light as well as the optical gain depends on the orientation of the resonator. Our measurements on separate confinement heterostructures on semipolar (11equation image2) and (10equation image2) GaN show that for laser resonators along the semipolar [11equation image] and [0equation image11] directions (i.e. the projection of the c-axis onto the plane of growth) the threshold for amplified spontaneous emission is lower than for the nonpolar direction and that the stimulated emission is linearly polarized as TE mode. For the waveguide structures along the nonpolar [1equation image00] or [11equation image0] direction on the other hand, birefringence and anisotropy of the optical gain in the plane of growth leads not only to a higher threshold but alsoto a rotation of the optical polarization which is not any more TE- or TM-polarized but influenced by the ordinary and extraordinary refractive index of the material. We observe stimulated emission into a mode which is linearly polarized in extraordinarydirection nearly parallel to the c-axis. (© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

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