Zusammenfassung
In der linearen Optik wird die Ausbreitung von Licht in Materie durch die Brechzahl n und die Dämpfungskonstante α beschrieben. Beide sind frequenzabhängige bzw. wellenlängenabhängige Größen, die unabhängig von der Strahlungsdichte des einfallenden Lichtes sind. Es gilt das Superpositionsprinzip, das besagt, daß Lichtsignale sich gegenseitig nicht beeinflussen und sich ungestört überlagern können. Die lineare Optik ist aber nur ein Grenzfall der Optik für kleine Strahlungsdichten. Bei großen Strahlungsdichten werden n und α von der Lichtleistung abhängig, und es tritt eine Vielzahl weiterer optischer Effekte auf, die die lineare Optik nicht kennt. Insbesondere gilt das Superpositionsprinzip nicht mehr. Licht kann durch Licht beeinflußt, gesteuert und geschaltet werden. Dies ist die Grundlage für die optische Signalverarbeitung, die in diesem Kapitel beschrieben wird.
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Weber, H.G. (2002). Nichtlineare Optik und optische Signalverarbeitung. In: Voges, E., Petermann, K. (eds) Optische Kommunikationstechnik. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-56395-9_16
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