Abstract:
The Ferroelectric high Tc superconductor RF Phase Shifter contains a ferroelectric medium and a film of a single crystal high Tc superconductor is used as the conductors. Between the ferroelectric medium and the input, there is a quarter-wave, dielectric or ferroelectric or the same material as used for the phase shifter, matching transformer. Between the ferroelectric medium and the output, there is a quarter-wave, dielectric, ferroelectric or the same material as used for the phase shifter, matching transformer. A bias field is connected across the top and bottom surfaces of the active ferroelectric medium. When a bias field is applied across the surfaces of the ferroelectric medium, the permittivity is reduced and as such the velocity of propagation is increased. This causes an increase in the effective electrical length of the phase shifter or a phase difference or time delay. Increasing the bias voltage increases the phase shift. The ferroelectric high temperature superconductor RF phase shifter may be embedded as a part of the monolithic integrated circuit. The ferroelectric high Tc superconductor RF phase shifter may be constructed of thin film and ferroelectric liquid crystal. The ferroelectric material is operated above its Curie temperature.
Abstract:
The ferroelectric limiter utilizes the bias voltage dependent dielectric constant property of a ferroelectric material. A main transmission line having a length of two or more half wavelengths at the operating frequency is used. A branch line is connected at one half wavelength away from one end of the transmission line. The branch line presents a very high impedance on the main transmission line at a low level of signal. The branch line contains a ferroelectric material. As the signal level increases, the dielectric constant of the ferroelectric material in the branch line changes. This reduces the impedance presented by the branch line on the main transmission line reducing the impedance of the main transmission line and the resulting output of the limiter. As the signal level increases, the impedance presented by the branch line on the main transmission line becomes increasingly smaller, further reducing the output of the of the limiter. Two designs of the limiter are presented. The limiter can be a part of a monolithic microwave integrated circuit (MMIC). The conductive coatings of the limiter can be a film of a single crystal high Tc superconductor material. The upper frequency limit of the ferroelectric limiter is determined by the relaxation frequency of the ferroelectric material such as 95 GHz for Strontium Titanate.
Abstract:
A design of equally loaded, under varying traffic load conditions, high efficiency power amplifiers for a multibeam communication system is presented. Output beam contains signals of only one beam corresponding to its input beam. Signals arriving at the feed elements for an input beam "b", of the 1 to N beams, corresponding to an input beam "b", arrive in phase and add together, while signals arriving at said feed elements for the output beam "b" corresponding to the remaining input beams arrive in antiphase and cancel one another by appropriate selection of two set of fixed input and output phase shifters. The output beams are shaped to produce a small reduction of power at the crossover point of adjacent beams. MMIC and high Tc superconducting designs, including the design of high Tc superconducting reflector antenna, are presented.
Abstract:
This invention pertains to monolithic filters of the band-pass or band-reject type which a single crystal ferroelectric material having an electric field dependent permittivity. The filters are comprised of: a first layer of a single crystal dielectric material; a second layer of a single crystal high T.sub.c superconductor material; a third layer of a single crystal ferroelectric material; and a fourth layer of high T.sub.c superconductive microstrip lines configured into the various filter circuits, including resonator circuits and transformer circuits. The filters are capable of operating at power levels up to 0.5 MW at a temperature slightly above the Curie temperature to avoid hysteresis.
Abstract:
A number of MMIC ferroelectric variable time delay devices are presented. Each embodiment has a microstrip configuration deposited on a ferroelectric film which is deposited on a high Tc superconductor substrate connected to the ground. A bias electric field changes the permittivity of the ferroelectric material. As a result, a variable time delay is obtained.
Abstract:
A design of equally loaded, under varying traffic load conditions, power amplifiers for a multibeam satellite is presented. Each output beam contains signals of only one beam corresponding to its input beam. The output beams are shaped to produce a small reduction of power at the crossover point of adjacent beams. MMIC and high Tc superconducting designs, including the design of high Tc superconducting reflector antenna, are presented.
Abstract:
A cylindrical cavity is loaded with a ferroelectric rod and is resonant at the dominant mode. The loaded cylidrical cavity is a band pass filter. As a bias voltage is applied across the ferroelectric rod, its permittivity changes resulting in a new resonant frequency for the loaded cylindrical cavity. The ferroelectric rod is operated at a temperature slightly above its Curie temperature. The loaded cylindrical cavity is kept at a constant designed temperature. The cylindrical cavity is made of conductors, a single crystal high Tc superconductor including YBCO and a single crystal dielectric, including sapphire and lanthanum aluminate, the interior conducting surfaces of which are deposited with a film of a single crystal high Tc superconductor. Embodiments also include waveguide single and multiple cavity type tunable filters. Embodiments also include tunable band reject filters.
Abstract:
To reduce the losses, high Tc superconductive waveguide filters are disclosed. There are two approaches to make the filters. In the first approach, all waveguide sections, irises, flanges are made of a single crystal high Tc superconductor. The single crystal is machined to the desired shape and size, the pieces are brazed and connected with flanges. In the second approach all waveguide sections, irises and flanges are made of a single crystal dielectric material the conducting surfaces of which are deposited with a film of a single crystal high Tc superconductor. The waveguide sections, irises and flanges are connected together by brazing or by a similar method. There are two basic types, (1) band pass and (2) band reject, of filters. In the band pass type, a series of resonators are placed one after another with a separation, typically, of three quarters of a wavelength between the centers of adjacent resonators. In the band reject filters, the resonators are in branch lines, i.e., on the broad wall of the main waveguide with a separation, typically, of three quarters of a wavelength between the centers of adjacent resonators.
Abstract:
An electronically controlled ferroelectric RF switch is an active medium formed from a ferroelectric material the permittivity, and as such the refractive index, of which may be varied by varying the strength of an electric field in which it is immersed. The ferroelectric RF switch includes the ferroelectric material having electrodes or conductors mounted thereon that are connected to an adjustable d.c. or a.c. voltage source. The switch may be placed in an RF transmission line that includes appropriate input and output impedance matching devices such as quarterwave transformers. The active medium of the RF switch is constructed of two prismatic structures of a ferroelectric material. When the two prisms are at the same zero bias voltage, then the RF energy passing through the switch is not deflected and the switch is in the OFF condition. Application of a bias voltage reduces the permittivity and the refractive index of the outer prismatic structure. The RF energy is refracted away from the normal at the interface between the prismatic surfaces. When the magnitude of the bias voltage is sufficiently high and the permittivity and the refractive index of the outer prismatic structure are sufficiently reduced, total internal reflection of the RF energy takes place at the boundary of the two prismatic surfaces and the switch is switched ON, and the RF energy appears on another port. The ferroelectric RF switch may be embedded as part of a microwave integrated circuit. The ferroelectric RF switch may be constructed of thin ferroelectric film. The copper losses may be reduced by using a high Tc superconductor material as the conducting surface. The ferroelectric material is operated in the paraelectric phase slightly above its Curie temperature. The switch is reciprocal between the conductive ports.
Abstract:
A coplanar waveguide is formed by a spiral with two arms. One arm is labelled 1, and the second arm is labelled 2. The arms labelled 1 and 2 are separated by equal distance. The spiral arms labelled 1 and 2 are formed by the deposition of a film of a conductor, a third layer, on a film 14 of a single crystal ferroelectric material, a second layer, which is deposited on a single crystal dielectric material, a first layer 1. Input is 10 and the output is 11. The CPW spiral arms labelled 1 and 2 forms a time delay device. When a bias voltage V is applied between the two spiral arms labelled 1 and 2 through a bias filter made of an inductor L and a capacitor C, the permittivity of the ferroelectric film between the two spiral arms labelled 1 and 2, or across the CPW, producing a change in the time delay. By the application of different levels of bias voltage between the two spiral arms labelled 1 and 2, different permittivity of the ferroelectric material are obtained and thus different changes in the time delay are obtained. Thus a variable time delay is obtained. Other delay embodiments are (1) meander line, (2) square shaped structure, (3) interdigital line, (4) parallel CPW.