The system components, performance, and calibration of two element radio interferometer operating at 8.33 mm wavelength are discussed. The interferometer employs a 5.5 m and a 3 m diameter antenna on an east-west baseline of 60 or 120 m, yielding fringe spacings at transit of 28 or 14 in. respectively. The broad intermediate frequency bandpass of 100 to 350 MHz and the system noise temperature of 500 K provide high sensitivity for the measurement of continuum sources. The interferometer has been used for high resolution studies of the planets and the Sun, and it is currently being adapted to study solar flare emissions at high spatial and time resolution
The theory and development of a VHF correlation radio interferometer for investigating ionospheric d...
Careful observations were made at 86.1 GHz to derive the absolute brightness temperatures of the Sun...
In April, 1981, radio telescopes at Dwingeloo (The Netherlands) and Onsala (Sweden) were used as a l...
The planets and their satellites were observed at high resolution at millimeter wavelengths with the...
The Caltech Millimeter-Wave Interferometer has recently begun observations at a wavelength of 2.6 mm...
A high-resolution microwave spectrometer has been developed by converting the Owens Valley solar int...
A new heterodyne interferometer for the atmospheric window from 9 to 12 microns was developed during...
Before contemplating an optical interferometer on the Moon one must first review the accomplishments...
Long-baseline interferometry achieves high resolution by using two or more widely separated radio te...
Three small antennas will be added to the OVRO interferometer to form a five-element solar-dedicated...
The Berkeley-Maryland-Illinois Array (BIMA) is briefly described in the context of solar observation...
When trying to uncover the properties of astronomical objects with high resolution an interferometer...
Resolution is the greatest constraint in observational astronomy. The Earth's atmosphere causes on o...
The two 90-foot steerable paraboloids of the Owens Valley Radio Observatory were used as a two-elem...
Radio astronomers, in common with many others who work with radio antennas, have always felt rather ...
The theory and development of a VHF correlation radio interferometer for investigating ionospheric d...
Careful observations were made at 86.1 GHz to derive the absolute brightness temperatures of the Sun...
In April, 1981, radio telescopes at Dwingeloo (The Netherlands) and Onsala (Sweden) were used as a l...
The planets and their satellites were observed at high resolution at millimeter wavelengths with the...
The Caltech Millimeter-Wave Interferometer has recently begun observations at a wavelength of 2.6 mm...
A high-resolution microwave spectrometer has been developed by converting the Owens Valley solar int...
A new heterodyne interferometer for the atmospheric window from 9 to 12 microns was developed during...
Before contemplating an optical interferometer on the Moon one must first review the accomplishments...
Long-baseline interferometry achieves high resolution by using two or more widely separated radio te...
Three small antennas will be added to the OVRO interferometer to form a five-element solar-dedicated...
The Berkeley-Maryland-Illinois Array (BIMA) is briefly described in the context of solar observation...
When trying to uncover the properties of astronomical objects with high resolution an interferometer...
Resolution is the greatest constraint in observational astronomy. The Earth's atmosphere causes on o...
The two 90-foot steerable paraboloids of the Owens Valley Radio Observatory were used as a two-elem...
Radio astronomers, in common with many others who work with radio antennas, have always felt rather ...
The theory and development of a VHF correlation radio interferometer for investigating ionospheric d...
Careful observations were made at 86.1 GHz to derive the absolute brightness temperatures of the Sun...
In April, 1981, radio telescopes at Dwingeloo (The Netherlands) and Onsala (Sweden) were used as a l...