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Der Halbleiterlaser

  • Chapter
Laser

Zusammenfassung

Wie in Gas- und optisch gepumpten Festkörperlasern kann auch in bestimmten Halbleitern eine Lichtemission induziert und bei Rückkopplung der entstehenden Strahlung ein Laser realisiert werden. Die wesentlichen Unterschiede, die eine gesonderte Behandlung des Halbleiterlasers erfordern, beruhen auf der Art der Elektronenzustände. Während diese bei den anderen Lasern in der Energieskala ein Spektrum schmaler Linien darstellen, sind beim Halbleiter breite Energiebänder vorhanden. Dieser Sachverhalt führt vor allem zu einer relativ großen Breite der spontanen Emissionslinie und damit nach der Schawlow-Townes-Bedingung (vgl. Gl. 7.3/5) zu einer sehr hohen Schwellenleistung für eine optische Anregung.

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  1. G. H. Winstel
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  1. Technischen Hochschule München, Deutschland

    W. Kleen (Direktor des European Space Research and Technology Center, Noordwijk, Niederlande, Honorarprofessor) & R. Müller (o. Professor, Direktor des Instituts für Technische Elektronik) (Direktor des European Space Research and Technology Center, Noordwijk, Niederlande, Honorarprofessor) &  (o. Professor, Direktor des Instituts für Technische Elektronik)

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Winstel, G.H. (1969). Der Halbleiterlaser. In: Kleen, W., Müller, R. (eds) Laser. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-87266-2_7

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