We report measurements of x-ray scattering cross sections for dense plasmas created by subjecting aluminum foils to strong laser-driven shocks. A narrow cone of quasimonochromatic x-rays at approximately 4.75 keV was used to probe the shocked part of the foil and scattered photons were detected with a CCD camera. The scattering cross section shows a clear peak, indicating diffraction from the plasma. Analysis and simulation of the data suggest that radiative heating and electron-ion energy exchange are important factors in the plasma production.
Well-known silicon micro fabrication techniques are used to create biocompatible abiotic glucose fuel cells, suitable for powering ultra-low-power bioelectronics on a silicon wafer. Measured continuous outputs of 2.3 µW/cm2 at 0.243V were achieved and maintained for a period of at least 48 hr with an open circuit voltage of 0.55V. Fabrication processes are discussed to address the difficulty in depositing and patterning Nafion separation membranes robustly and in the creation of a uniform carbon nanotube mesh catalyst.
Experiments have been carried out to investigate the polar distribution of atomic material ablated during the pulsed laser deposition of Cu in vacuum. Data were obtained as functions of focused laser spot size and power density. Thin films were deposited onto flat glass substrates and thickness profiles were transformed into polar atomic flux distributions of the form f ͑͒ϭcos n . At constant focused laser power density on target, Iϭ4.7Ϯ0.3ϫ10 8 W/cm 2 , polar distributions were found to broaden with a reduction in the focused laser spot size. The polar distribution exponent n varied from 15Ϯ2 to 7Ϯ1 for focused laser spot diameter variation from 2.5 to 1.4 mm, respectively, with the laser beam exhibiting a circular aspect on target. With the focused laser spot size held constant at ϭ1.8 mm, polar distributions were observed to broaden with a reduction in the focused laser power density on target, with the associated polar distribution exponent n varying from 13Ϯ1.5 to 8Ϯ1 for focused laser power density variation from 8.3Ϯ0.3ϫ10 8 to 2.2Ϯ0.1ϫ10 8 W/cm 2 , respectively. Data were compared with an analytical model available within the literature, which correctly predicts broadening of the polar distribution with a reduction in focused laser spot size and with a reduction in focused laser power density, although the experimentally observed magnitude was greater than that predicted in both cases.
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