Abstract
Firstly developed to explain the behaviour of electrons scattered by excited atoms [1], Fano’s model has later become a cornerstone in modern physics, finding applications in such diverse fields [2] as ultracold gases, Bose-Einstein condensates, semiconductors, quantum dots and plasmonic nanostructures. Fano resonances are generally observed, as a single-particle phenomenon, when quantum interference occurs between different decay channels: this results in a characteristic broadening and an asymmetric deformation of the natural line shape.
© 2015 IEEE
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