Collective optical excitation of interacting localized electrons. Metzner, C. & Döhler, G., H. Physical Review B, 60(15):11005-11013, AMER PHYSICAL SOC, ONE PHYSICS ELLIPSE, COLLEGE PK, MD 20740-3844 USA, 10, 1999. ![Collective optical excitation of interacting localized electrons [pdf]](https://bibbase.org/img/filetypes/pdf.svg "pdf")
Paper ![Collective optical excitation of interacting localized electrons [link]](https://bibbase.org/img/filetypes/link.svg "link")
Website abstract bibtex We investigate theoretically the role of dynamic screening in the intersubband absorption process of a quasi-two-dimensional (quasi-2D) electron gas with in-plane localization caused by a strong disorder potential. Due to a correlation effect in the single-particle spectrum this system is equivalent to an array of randomly distributed, localized oscillators, which are mutually coupled by the electron-electron Coulomb interaction. In the limit of low-electron density, a broad absorption spectrum reflects the disorder-induced distribution of the individual transition energies. For increasing electron filling factor we find a depolarization-type blueshift similar to the case of quasi-2D systems without disorder. Simultaneously a dramatic line narrowing is observed, indicating a collective response of the interacting localized electrons. In this collective mode large clusters of mutually phase-adapted oscillators are formed in the layer plane. Our results are relevant for the interpretation of intraband absorption experiments in all kinds of disordered quasi-2D systems and in dense arrays of artificial quantum dots. A similar effect is expected for inter-Landau-level transitions in magnetically quantized 2D systems. [S0163-1829(99)06539-X].
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abstract = {We investigate theoretically the role of dynamic screening in the intersubband absorption process of a quasi-two-dimensional (quasi-2D) electron gas with in-plane localization caused by a strong disorder potential. Due to a correlation effect in the single-particle spectrum this system is equivalent to an array of randomly distributed, localized oscillators, which are mutually coupled by the electron-electron Coulomb interaction. In the limit of low-electron density, a broad absorption spectrum reflects the disorder-induced distribution of the individual transition energies. For increasing electron filling factor we find a depolarization-type blueshift similar to the case of quasi-2D systems without disorder. Simultaneously a dramatic line narrowing is observed, indicating a collective response of the interacting localized electrons. In this collective mode large clusters of mutually phase-adapted oscillators are formed in the layer plane. Our results are relevant for the interpretation of intraband absorption experiments in all kinds of disordered quasi-2D systems and in dense arrays of artificial quantum dots. A similar effect is expected for inter-Landau-level transitions in magnetically quantized 2D systems. [S0163-1829(99)06539-X].},
bibtype = {article},
author = {Metzner, C. and Döhler, G. H.},
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