A narrower illumination spot could be realized, for example, by using a miniature cylindrical lens at the distal end of the illumination fiber, and higher spectral efficiency could be achieved by using course spectral dispersion in the illumination by further adding a diffraction grating; both techniques could potentially allow several-fold improvement in SNR.
However, with careful design of the active layer structure, InGaN blue LDs with high efficiency and temperature-stable operation are expected to be realized for potential use in LD-based solid-state lighting, display, and communication applications.
The experimental results show that a reliable autonomous RE system can be realized for such seasonal energy sources, using stored hydrogen as the long-term energy buffer, and that utilizing the electrolyzer oxygen by-product as oxidant in the fuel cell increases system performance significantly.
Experiments show that significant drag reductions may be realized for circular cylinders in cross-flow by using grooves, even at very shallow relative groove depths.
An IBAD buffered substrate using IBAD-MgO layer (CeO2/LMO/IBAD-MgO/Hastelloy C276) was developed and a high production rate of 24 m/h was realized for IBAD-MgO layer using a small ion gun system with the area of 6 × 22 cm22
High-temperature operation, which is realized for the first time by using an IL, can take full advantage of the high capacity of HC even at a very high discharge rate of 1000 mA (g-HC −1: g-HC −1charge capacitheis 230 mAh (g-HC)−1 at 90 °C andischarge(g-Hcapacity25 °C.
Due to less cellular toxicity of the substrate using the microemulsion system, the repeated-cycle bioconversion based on microemulsion using recycled cells was realized for the first time, and the overall 6-cycle production (41.5 g from 60 g DHEA) was 4.3 times that of the traditional method.
A possible implementation of endoscopic spectrally encoded spectral imaging could be realized by using two imaging modes: one for real-time monochromatic imaging for in-body navigation, and a second, slow and linear probe motion for acquiring high spectral or color fidelity.
Two-color STED imaging can be realized by using either different STED wavelengths for the two fluorophores or the same wavelength for both.
Several examples are presented that illustrate the possible improvements that can be realized using the new algorithm for problems relevant to plasma simulation.
