Laser Action from Terbium Trifluoroacetylacetonate in P-Dioxane and Acetonitrile at Room Temperature
Laser activity from terbium trifluoroacetylacetonate in p-dioxane and acetonitrile at room temperature
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Laser activity from terbium trifluoroacetylacetonate in p-dioxane and acetonitrile at room temperature
Laser holography combined with schlieren techniques to measure ray deviations in optically inhomogeneous field of transient phenomenon
Line-narrowing effect induced by laser radiation applied to measurements of isotope shifts for two optical transitions in neon
Microwaves and laser links for spacecraft-earth communications noting limitations by external noise effects, atmospheric turbulence, fabrication tolerances, etc
Electronic, vibrational and rotational temperatures in laser-produced flames measured spectroscopically
Gaseous chemical reaction dynamics analyzed with monochromatic laser light-induced photocatalysis
Evaporation of thin films of high melting point materials by focused laser beam and reflectance and relative transmittance in vacuum UV
Direct excitation in argon gas from metastable state to upper laser state compared with two-step excitation
Continuous wave laser ground-space-ground experiment in conjunction with Explorer XXII SATELLITE tracking
Frequency stabilization of laser oscillator against reference laser amplifier, noting residual AM effects
Q-switched laser use as light source for photographing droplets in spray containing fluorescent dye excited by second harmonic of ruby light
Laser lines observation in Freon-He mixtures in CW gas discharge
Holographic interferometry with UV light from KDP crystal generating second harmonic of Q switched ruby laser red output, noting optical path length sensitivity
Tunable optical parametric oscillator using argon laser CW output as pump and lithium niobate as nonlinear crystal
High speed flowing gas system provides uniform mixing in short times compared to flow transit times and carbon dioxide vibrational relaxation times. This system minimizes the effects of surrounding surfaces and provides a uniformly high gain that is independent of dimensions transverse to the flow direction.
An optical radar for detecting targets in natural waters was built and tested in the Gulf of Mexico. The transmitter consists of a Q switched neodymium glass laser, with output amplified and doubled in KDP to 0.53 micrometer wavelength. The receiver incorporates a noval optical spatial filter to reduce the dynamic range required of the photodetector to a reasonable value. Detection of targets to a depth of 26 meters (84 feet) was achieved with a considerable sensitivity margin. The sensitivity of the radar is highly dependent on the optical attenuation coefficient. In general, measured returns fell between the values predicted on the basis of monopath and multipath attenuation. By means of simple physical arguments, a radar equation for the system was derived. To validate this theoretical model, measurements of optical attenuation and of water surface behavior were also instrumented, and some of these results are given.
Several methods of using lasers to measure atmospheric temperature profiles were described. Mason's suggestion was analyzed here to assess its capabilities for various lidar configurations. Temperatures were inferred from a measure of the Boltzmann distribution of rotational states in one of the vibrational bands of O2. Differential absorption was measured using three tunable, narrowband pulsed lasers. The outputs of two were tuned to wavelengths at the centers of absorption lines at either end of a particular branch in the band. The third wave-length was in a region of no absorption; its lidar return measured only the atmospheric backscatter, and therefore allowed calculations of the absorption coefficients at the other two wavelengths as a function of altitude. From the ratio of the two line absorption coefficients plus a priori knowledge of the line parameters, the temperature-altitude profile were calculated.
In Mason's method (1975) atmospheric temperatures are inferred from a measure of the Boltzmann distribution of rotational states in one of the vibrational bands of O2. Differential absorption is measured using three tunable, narrowband pulse lasers. The outputs of two are tuned to wavelengths at the centers of absorption lines at either end of a particular branch in the band; the third wavelength is in a region of no absorption. The temperature-altitude profile can be calculated from the ratio of the two line absorption coefficients plus a priori knowledge of the line parameters. In the present paper, computer simulations of various lidar configurations are made, using different line pairs in the atmospheric bands of O2 (approximately 630, 690, and 760 nm). Simulated results are presented for temperature profiles measured from a Space Shuttle lidar.