Development of electronically tunable converters in the millimeter wave range final report, 16 jul. 1963 - 16 nov. 1964
Electronically tunable converter in millimeter wave range
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Electronically tunable converter in millimeter wave range
Tunable phase detector for short term frequency stability measurements
Tunable birefringent Fabry-Perot interferometer used in study of solar magnetic fields, using Zeeman effect
Tunable coupling of open waveguide type for semiconfocal Fabry-Perot cavity gives high transmission and high Q
Optical fluorescence, thermally tunable over significant portion of visible and near IR SPECTRUM, from phase-matched parametric system
Repetitively pulsed tunable ruby laser for high resolution absorption spectroscopy and selective photochemical excitation, using solid etalon for mode control
Electron beam pumped laser action in selenium and tellurium with applications for tunable backward parametric oscillations
Electronically tunable lithium niobate optical filter utilizing collinear acousto-optic diffraction in anisotropic medium
Tunable optical parametric oscillators including Gaussian beams amplification, threshold, tuning techniques, spectral output, etc
Fabry-Perot interferometer series as tunable optical narrow passband filter with high spectral and angular resolution, discussing performance in solar magnetograph
Voltage tunable Gunn effect semiconductor for microwave generation
Negative ions photodetachment by continuously tunable laser and ion cyclotron resonance spectrometer
Newly developed Gunn oscillator is three-terminal device which consists of piece of gallium arsenide with source, drain, and gate contacts. Voltage tunable three-terminal device does not require bulky resonant cavity and allows oscillation frequency to be rapidly tuned with simple circuitry.
Consideration of the application of the measurement of resonance fluorescence radiation excited by tunable laser radiation to the detection of atomic, molecular, and ionic species in the upper atmosphere. The species considered are N2, N2(+), NO, NO(+), O2(+), CO, CO(+), CH, Na, K, and Ca. Calculations of the resonance scattering cross sections, photon returns, and signal-to-noise ratios are given for these species for a range of conditions. Based on a probing altitude of 100 km, the detections of N2, NO, CO, CH, O2, and the trace metals appear feasible with state-of-the-art systems and within the concentration range present in the atmosphere.
A tunable laser apparatus is reported with a first wavelength selective reflector and a second wavelength selective reflector forming one end of an optical cavity, and a third wavelength selective reflector forming the other end of an optical cavity. A first lasable dye solution develops radiation of a wavelength selected by the first reflector and a second lasable dye solution develops radiation of a wavelength selected by the second reflector and a non-linear mixing crystal disposed within the optical cavity. The selected radiation is passed through the nonlinear mixing crystal causing it to develop radiation of a third wavelength which is transmitted out of the optical cavity through the third reflector.
Apparatus in which laser wavelengths of two dyes are mixed in intracavity, nonlinear crystal provides intense source of coherent laser radiation which is tunable from visible through infrared wavelengths of electromagnetic spectrum.
Atmospheric transmission of high energy CO2 lasers is considerably improved by high pressure operation which, due to pressure broadening, permits tuning the laser lines off atmospheric absorption lines. Pronounced improvement is shown for horizontal transmission at altitudes above several kilometers and for vertical transmission through the entire atmosphere. Applications of tunable high pressure CO2 lasers to energy transmission and to remote sensing are discussed along with initial efforts in tuning high pressure CO2 lasers.
A tunable high-repetition-rate oscillator-amplifier dye-laser system is reported. The dye laser described was longitudinally pumped with the second harmonic of a Nd-YAG laser operating at 10 Hz. Using three Faraday-Perot etalons and pressure tuning, a maximum fundamental output power of the order of 6 MW with a corresponding spectral width of less than 0.003 nm at 564 nm was obtained. The fundamental at 564 nm was frequency doubled to give a maximum power level of 0.6 MW of second-harmonic output power with a spectral width less than 0.0015 nm at 282 nm. Frequency stability could be maintained to within approximately 15% of the line-width.