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Implemented in double precision arithmetic in a PC/286/87 personal computer, this scheme is shown to achieve about ten correct digits in the first five natural frequencies of uniform beams (six correct digits for modes as high as 20) and to agree satisfactorily with exact and approximate natural frequencies of several types of nonuniform beams reported by other authors.
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However, defining a slotted block geometry which guarantees sufficient tuned frequency isolation from nearby modes as well as high amplitude and amplitude uniformity, is not straightforward.
For the injected carrier density of 5×1012/cm2, the optimized optical gain within TE mode is as high as ~9000/cm at the wavelength of ~1.95 µm, thus providing a very important alternative material system for the generation of SWIR wavelength region.
For the injected carrier concentration of 5 × 1012/cm2, the optimized optical gain within TE mode is as high as ∼9000/cm at the wavelength of ∼1.95 μm, thus providing a very important alternative material system for the generation of SWIR wavelength region.
Finally, it is shown that interaction of the guided light improves extraction of both lower order modes as well as higher order modes, which enhance LED efficiency.
This paper discusses new hybrid MS instruments that can perform novel scan modes as well as high-resolution mass spectrometers (HRMS) that finally seem to be able to overcome, or at least significantly reduce, their weaknesses in quantitative applications.
Using the CBA mode as high resolution imaging mode also enables to measure with simultaneously high lateral and mass resolution in burst mode as demonstrated in Section 5.
It is demonstrated that internal resonances occur between the first and higher order modes, as well as between the second and higher order modes.
For complex likelihood functions with multiple modes, this number may be as high as 10 000, and for a single mode as low as 200.
When choosing "outdoors mode", WhiteMagic's brightness can be boosted from 470 cd/m² to an impressive 1,000 cd/m², while power consumption of the backlight in this mode (300mW) stays about as high as that of conventional screens.
These lasers exhibit low-temperature threshold current densities of 860A/cm2 in pulsed mode and output power as high as 6 W per facet (12 W total).
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