Zusammenfassung
Wie in Kap. 1 und 4 dargelegt, besteht der Laser aus einem aktiven Medium, in dem Licht einer oder mehrerer Wellenlängen verstärkt wird, und einem Resonator (s. Kap. 3), in dem sich das aktive Medium befindet. Durch den Resonator wird das verstärkte Licht bei jedem Umlauf wieder in das verstärkende Medium zurückgekoppelt. Bei Pumpleistungen oberhalb des Schwellenwerts erhöht sich die Schwingungsenergie, bis die ihr proportionale Summe aus Verlusten (auf Grund von Streuung, Beugung und Absorption) und ausgekoppelter Leistung gleich dem Energiegewinn durch die gegebene Verstärkung ist. Die Verstärkung geschieht durch induzierte Emission, auf Kosten der Anregungsenergie aktiver Atome.
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Gürs, K. (1969). Der optisch gepumpte Festkörperlaser. In: Kleen, W., Müller, R. (eds) Laser. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-87266-2_5
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