New PDF release: Das Bild der modernen Physik

By Pascual Jordan.

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1. Introduction . . . . . . . . . . . . . . 2. Near-Field Optics . . . . . . . . . . . . 3. Theoretical Description of Near-Field Optics of Semiconductor Nanostructures . . . . . . . . . . . . . 4. Near-Field Probes . . . . . . . . . . . . 5. Probe-to-Sample Distance Control . . . . . . . . . 6. Low-Temperature Near-Field Microscopy . . . . . . . 7. Temporally and Spatially Resolved Near-Field Spectroscopy . . . . IV. Stationary Near-Field Spectroscopy of Semiconductor Nanostructures .

Because of the small density of states and strong dispersion of the lh band, the absorption changes seen in cocircular geometry essentially originate from the carriers generated involving the hh band. Therefore, this situation is adapted in our measurements in order to keep the degree of complexity in the spectra as low as possible. To demonstrate the opposite effect of countercircularly polarized excitation and test pulses, we show the transient spectrum obtained in this 1 Ultrafast Electron—Phonon Interactions 21 geometry in Fig.

References . . . . . . . . . . . . . . . . . . 39 41 41 43 46 46 49 . . . 53 56 58 59 61 . 65 65 . 66 79 . . 79 89 98 98 I. Introduction Man-made artificial semiconductor nanostructures allow a spatial confinement of electrons and holes on a length scale comparable to their de Broglie wavelengths, resulting in a quantization of the electronic band structure. Parameters such as dimensionality and size of the structures, material composition, and/or strain of the crystal lattice determine the type 39 Copyright 2001 by Academic Press All rights of reproduction in any form reserved.

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