Interferometer direction sensor Patent
Michelson interferometer with photodetector for optical direction sensing
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Michelson interferometer with photodetector for optical direction sensing
Servo system for retroreflector of Michelson interferometer
Influence of atmospheric refraction on minitrack interferometer system and correction procedures for computation accuracy
Design and development of optical interferometer with laser light source for application to schlieren systems
Digital sensor for counting fringes produced by interferometers with improved sensitivity and one photomultiplier tube to eliminate alignment problem
Electron density measurement of negative glow plasma with E-band Fabry-Perot interferometer using flat plate technique
Test plans for conducting very long baseline interferometer experiments using Applications Technology Satellites 3 and 5
Analysis of concept of spin-stabilized synchronous satellite carrying interferometer transmitting CW signals in L-band
Satellite radio interferometer multipath reflections effect on accuracy
Iterative technique using continuous gas laser for alignment of Mach-Zehnder interferometer for monochromatic and white light fringes
Michelson interferometer onboard Nimbus 4 satellite for recording earth IR emission spectrum
Water vapor emission map at 22 GHz from W 49, using three-station long baseline radio interferometer data
Solar Fe XIV 5303 coronal line isolation, using solid Fabry-Perot interferometer as monochromator
Exospheric evening temperature behavior data, using Fabry-Perot interferometer measurements of atomic oxygen line Doppler broadening
Mars IR spectra with Connes-type interferometer, noting atmospheric absorption and albedo drop due to surface water
The theory and development of a VHF correlation radio interferometer for investigating ionospheric disturbances are discussed. The system was developed to receive signals from the geostationary Applications Technology Satellites. Amplitude and phase variations of the signal passing through the ionosphere can be detected by this instrument. The system consists of two superheterodyne receivers separated by a distance known as the baseline of the system. Since the system is a phase sensitive instrument, the local oscillators of the two receivers must be phase coherent. This is accomplished by using phase-locked loops for generating the local oscillators. The two signals from the separate receivers are cross-correlated by multiplying the two signals together and then time averaging the result. The sensitivity of the instrument is increased by off-setting one of the local oscillators by a small amount.
During 1971, a series of very long baseline interferometer observations were made of the C-band (6 cm) radio signals from the ATS-3 communications satellite which is in a synchronous, near-equatorial orbit. The first series of observations were conducted during May-June 1971 from Rosman, North Carolina (NASA/ATS Station 85' dish) and Mojave, California (NASA/ATS Station, 40' dish). The second series of observations were conducted during August-September, 1971 from Rosman, North Carolina (NASA/ATS Station, 85' dish), Owens Valley, California (Cal Tech, 130' dish) and Agassiz, Massachusetts (SAO Agassiz Radio Observatory, 84' dish). The ATS-3 Spacecraft position was determined with a precision of 70-100 meters and its velocity with a precision of less than a mm/sec. The ATS-3 orbital elements were computed using the GEODYN program and the derived values are consistent with those derived from conventional tracking data.
Demonstration that the use of the Fabry-Perot interferometer as a filter with transmission windows occurring at regular intervals in wave numbers provides a highly sensitive method for detection of atmospheric gases using their rotational Raman spectra excited by a suitable laser. Some of the operating advantages include signal gains of several orders of magnitude, a simple direct interpretation of the results in terms of the density and types of the gaseous constituents, size and weight reductions from conventional apparatus, ease of operation, and relative freedom from interference from other molecules in the scattering volume. This method is compared with the techniques that have been discussed in the literature by other workers in the field.