Observation of an enhanced Lamb dip with a pure Xe gain cell inside a 3.51-micron He-Xe laser
He-Xe laser with pure Xe-136 gain cell inside cavity, observing enhanced Lamb dip in power output vs frequency curve
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He-Xe laser with pure Xe-136 gain cell inside cavity, observing enhanced Lamb dip in power output vs frequency curve
Stable adaptive control with gain constraints
High gain antenna acquisition problem during Apollo 13 flight
Numerical integration of equations for vibrational relaxation and radiative gain in expanding flows of anharmonic gas oscillators
Comb type traveling wave maser amplifier for improved high gain broadband output
Nonlinear filter construction and performance evaluation, using deterministic filter gains
Gas proportional counting system gain stabilization, using feedback loop radioactive X ray emitter and correction signal
Low gain microwave amplifier cascade DC to RF conversion efficiency analysis
Liapunov design technique for model reference adaptive control systems with feedback and prefilter adjustable gains
Intense superradiant emission in HF and DF molecules high gain IR transitions, examining spectral distributions with pneumatically tuned Fabry-Perot interferometer
CW carbon dioxide gasdynamic laser gain for mixture of carbon dioxide, nitrogen and helium
Substrate emitter monolithic inverted transistor structure for low-power high-current gain application
Brayton cycle 2-15 kW power system for space application and potential gains from component improvements, discussing current status
Critical reappraisal of the bias dependence of the dc and small-signal ac current gain factors of planar bipolar transistors over a wide range of currents. This is based on a straightforward consideration of the three basic components of the dc base current arising due to emitter-to-base injected minority carrier transport, base-to-emitter carrier injection, and emitter-base surface depletion layer recombination effects. Experimental results on representative n-p-n and p-n-p silicon devices are given which support most of the analytical findings.
A lightweight small high gain antenna which is capable of being packaged in a collapsed form and automatically expanded when in use is described. The antenna includes a cylindrical housing having a rod with a piston adjacent to one end extending through it. Attached to the outer end of the rod in a normally collapsed state is a helical wire coil. When the gas producing means is activated the piston and rod are shifted outwardly to expand the wire coil. A latch is provided for holding the helical coil in the expanded position.
A new method is demonstrated with which near-field antenna gain correction factors can be calculated directly from measured far-field pattern data by using a spherical wave expansion of the pattern. This eliminates the need for any assumptions regarding antenna aperture field distributions. For illustration, the method is applied to the case of a horn antenna. A comparison of the calculation results with direct measurement data shows an agreement within 0.03 dB. The method, when compared to the method used by Chu and Semplak (1965), is found to show similar agreement.
Davison (1970) has demonstrated that it is possible to assign max (m, p) poles of a linear time-invariant controllable and observable multivariable system arbitrarily close to desired locations by using constant gain output feedback. A new proof of Davison's theorem on pole placement is developed, and a system design procedure is described which offers some advantages over Davison's method. It is shown that in some cases more than max (m, p) poles can be assigned arbitrarily, and a least square design procedure is proposed to approximate the desired pole locations when it is not possible to place all the poles.
Expressions are developed for the gain of a centrally obscured, circular optical antenna used as the collecting and focusing optics in a laser receiver, involving losses due to (1) incoming light blockage by central obscuration, (2) energy spillover at the detector, and (3) the effect of local oscillator distribution in the case of heterodyne or homodyne detection. Numerical results are presented for direct detection and for three types of local oscillator distribution (uniform, Gaussian, and matched).