72 research outputs found

    Correlation Between Bulk Morphology and Luminescence in Porous Silicon Investigated by Evaporation Induced Pore Collapse

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    AbstractWe use a combination of scanning electron microscopy, laser scanning confocal microscopy and luminescence spectroscopy to correlate the emission properties of anodized porous silicon (PS) with film morphology in samples that have undergone evaporation induced collapse of the underlying porous structure. Several PS samples were investigated as a function of the current density (J) and total etch time, while the total charge (Q) injected per unit area (and the total Si removed) was kept constant during etching. From this data two classes of PS samples emerge. Porous silicon samples produced at high current density have a 3-dimensional pore network with a narrow distribution of blue-green emitting chromophores. In contrast, low current density samples form a 2-dimensional pore network normal to the Si substrate with larger chromophores and exhibit broad red luminescence.</jats:p

    Ultrafast Dynamics of Lasing Semiconductor Nanowires

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    Semiconductor nanowire lasers operate at ultrafast timescales; here we report their temporal dynamics, including laser onset time and pulse width, using a double pump approach. Wide bandgap gallium nitride GaN , zinc oxide ZnO , and cadmium sul amp; 64257;de CdS nanowires reveal laser onset times of a few picoseconds, driven by carrier thermalization within the optically excited semiconductor. Strong carrier amp; 8722;phonon coupling in ZnO leads to the fastest laser onset time of amp; 8764;1 ps in comparison to CdS and GaN exhibiting values of amp; 8764;2.5 and amp; 8764;3.5 ps, respectively. These values are constant between nanowires of di amp; 64256;erent sizes implying independence from any optical in amp; 64258;uences. However, we demonstrate that the lasing onset times vary with excitation wavelength relative to the semiconductor band gap. Meanwhile, the laser pulse widths are dependent on the optical system. While the fastest ultrashort pulses are attained using the thinnest possible nanowires, a sudden change in pulse width from amp; 8764;5 to amp; 8764;15 ps occurs at a critical nanowire diameter. We attribute this to the transition from single to multimode waveguiding, as it is accompanied by a change in laser polarization
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