Communications in the regenerated cellulose layer. We suppose that the hydrophobic disiloxane segregates from the hydrophilic cellulose film to the gas phase.The X-ray reflection analysis (Fig. 2 (bottom)) of the regenerated cellulose film exhibits Kiessig fringes, but no Bragg signal. From the periodical intensity modulations one calculates a film thickness of 79 A and a surface roughness of 8 A. Although the film thickness decreased by 60 YO during
We analyzed the intrinsic defects and the n-type-carrier concentration generated by nitrogen ion implantation in n-type GaN by deep-level-transient spectroscopy and by capacitance–voltage measurements, respectively. The samples were grown on sapphire by metalorganic vapor-phase epitaxy. Nitrogen implantation with different ion doses and postimplantation rapid-thermal annealing (RTA) were investigated. We observed a growing n-type-carrier concentration and increasing defect concentration with increasing nitrogen ion implantation doses. After RTA the concentration of free carriers and deep levels as found in the as-grown state are restored. We also address contrarily seeming results from measurements of sheet resistance after N implantation published recently.
Self-assembled growth in combination with prepatterning yields ordered lines of Ge islands on a planar Si (001) surface. The self-assembled Ge nanostructures are grown on top of a 15-period Si/SiGe superlattice, which is deposited on a prepatterned Si substrate. The pattern consists of 10 nm deep trenches with a period of 250 nm. The superlattice translates the surface modulation of the substrate into a strain-field modulation at the growth front of the superlattice. This strain field modulation provides the template for the ordered nucleation of self-assembled Ge islands. Our method gives rise to the long-range ordering of perfectly passivated nanostructures and can in principle be applied to any other strained material system.
In a carefully selected set of strained In"Ga& As/CxaAs quantum-well structures, we have studied experimentally and theoretically the competition between carrier collection from the GaAs barrier into the quantum wells and the inverse process, the thermal activated emission out of the wells into the barrier. Analyzing the temperature dependence of time-integrated photoluminescence measurements, we found excitons or electron-hole pairs to be emitted out of the well. A different sample geometry is used to demonstrate the importance of the barrier properties in the equilibrium of capture and thermal emission. Time-resolved experiments allow the determination of the typical time constants, namely the radiative and the nonradiative recombination lifetime as well as the emission time. A hydrodynamic model, including the diffusion in the barrier and the carrier capture and emission via LO phonons, was developed for a quantitative description of our experiments. With use of the experimental time constants, an excellent agreement between the time-integrated experiments and theory was found, giving evidence of the applicability of our model.
We establish rate equations to describe Auger carrier capture kinetics in quantum dot structures, calculate Auger capture coefficients for self-assembled quantum dots, and analyze Auger capture kinetics using these equations. We show that Auger capture times can be of the order of 1–100 ps depending on barrier carrier and dot densities. Auger capture rates depend strongly on dot diameters and are greatest at dot diameters of about 10–20 nm.
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