Abstract: Bulk acoustic wave resonators are presented. Such resonators typically operate based on a dynamic nonuniform effective piezoelectricity in composite multilayer ferroelectrics with large electrostriction coefficients, like barium strontium titanate (BST). Harmonic resonance modes of a multilayer bulk acoustic wave resonator can be selectively excited with an electromechanical coupling coefficient equal to the fundament mode, which is contrary to the trend K2?1/n2 exhibited by conventional piezoelectric bulk acoustic resonators. Such a resonator allows for the design of a new class of band-switching filters.

Abstract: A nonlinear resonator is presented that enhances the bandwidth while providing high resonance amplitude. The nonlinear resonance circuit is comprised of an inductor electrically coupled to a capacitor, where either the inductor or capacitor is nonlinear. Response of the nonlinear resonance circuit to an excitation signal is described by a family of second-order differential equations with cubic-order nonlinearity, known as Duffing equations. In one aspect, the nonlinear resonator is implemented by a nonlinear dielectric resonator.

Abstract: A nonlinear resonator is presented that enhances the bandwidth while providing high resonance amplitude. The nonlinear resonance circuit is comprised of an inductor electrically coupled to a capacitor, where either the inductor or capacitor is nonlinear. Response of the nonlinear resonance circuit to an excitation signal is described by a family of second-order differential equations with cubic-order nonlinearity, known as Duffing equations. In one aspect, the nonlinear resonator is implemented by a nonlinear dielectric resonator.

Abstract: A nonlinear resonator is presented that enhances the bandwidth while providing high resonance amplitude. The nonlinear resonance circuit is comprised of an inductor electrically coupled to a capacitor, where either the inductor or capacitor is nonlinear. Response of the nonlinear resonance circuit to an excitation signal is described by a family of second-order differential equations with cubic-order nonlinearity, known as Duffing equations.

Abstract: A circuit for generating a negative group delay (NGD). The circuit comprises one or more electrical components, at least one of which has an input impedance that is sufficient for the electrical component(s) to generate an NGD. In an embodiment, the circuit comprises antenna that is configured to radiate an electrical signal delivered thereto and generate an NGD. The antenna has an input impedance sufficient for the antenna to generate the NGD. In another embodiment, the circuit comprises an amplifier that is configured to amplify an electrical signal delivered thereto and generate an NGD. In such an instance, the amplifier has an input impedance and either the amplifier or one or more matching circuits thereof has a quality factor sufficient to generate the NGD.

Abstract: An adaptive power distribution system is presented for extending the dynamic range of AC/RF rectifiers. The power distribution system distributes the AC/RF input power amongst several different rectifier cells adaptively based on input power level. Consequently, high rectification efficiency can be maintained over a very wide dynamic range.

Abstract: An adaptive power distribution system is presented for extending the dynamic range of AC/RF rectifiers. The power distribution system distributes the AC/RF input power amongst several different rectifier cells adaptively based on input power level. Consequently, high rectification efficiency can be maintained over a very wide dynamic range.

Abstract: A nonlinear resonator is presented that enhances the bandwidth while providing high resonance amplitude. The nonlinear resonance circuit is comprised of an inductor electrically coupled to a capacitor, where either the inductor or capacitor is nonlinear. Response of the nonlinear resonance circuit to an excitation signal is described by a family of second-order differential equations with cubic-order nonlinearity, known as Duffing equations.

Abstract: A circuit for generating a negative group delay (NGD). The circuit comprises one or more electrical components, at least one of which has an input impedance that is sufficient for the electrical component(s) to generate an NGD. In an embodiment, the circuit comprises antenna that is configured to radiate an electrical signal delivered thereto and generate an NGD. The antenna has an input impedance sufficient for the antenna to generate the NGD. In another embodiment, the circuit comprises an amplifier that is configured to amplify an electrical signal delivered thereto and generate an NGD. In such an instance, the amplifier has an input impedance and either the amplifier or one or more matching circuits thereof has a quality factor sufficient to generate the NGD.

Abstract: Techniques for the design of low cost, low complexity phased arrays are described. The techniques allow control of the phase progression in the entire phased array by using only one phase shifter for a bank of arrays. In some examples, the phased array includes directional couplers, amplifying stages, power combiners and a phase shifter. The phase shifter may be of various kinds, including simple and compact phase shifters formed of varactor diodes and inductors or transmission lines.

Abstract: Techniques for the design of low cost, low complexity phased arrays are described. The techniques allow control of the phase progression in the entire phased array by using only one phase shifter for a bank of arrays. In some examples, the phased array includes directional couplers, amplifying stages, power combiners and a phase shifter. The phase shifter may be of various kinds, including simple and compact phase shifters formed of varactor diodes and inductors or transmission lines.

Abstract: A phased array for controlling a radiation pattern of an array of antennas includes a plurality of antenna ports, a first tunable element connected in series between each respective pair of adjacent antenna ports, and a second tunable element connected in parallel with each respective antenna port. The phased array provides progressive phase differences between successive antenna ports Equal amplitude of the signal can be maintained at each antenna. An equal amount of successive phase change can be provided in a signal at each antenna. A direct current source connectible to at least one input port can include an alternating power source through a matching circuit, such as a quarter-wave transformer The first and second tunable elements can be either an inductor or a capacitor, and/or can be in combination with transmission lines separating each respective antenna from a successive antenna by desired fraction of a wavelength.

Abstract: Disclosed herein is a front-end device for a phased array system. The front-end device includes an array of horn antennas, a first set of transmission lines coupled to the horn antenna array for a first polarization, a second set of transmission lines coupled to the horn antenna array for a second polarization orthogonal to the first polarization, and a plurality of L-shaped excitation elements. Each L-shaped excitation element of the plurality of L-shaped excitation elements couples a transmission line from each of the first and second sets of transmission lines to a respective horn antenna of the horn antenna array.

Abstract: Disclosed herein is a front-end device for a phased array system. The front-end device includes an array of horn antennas, a first set of transmission lines coupled to the horn antenna array for a first polarization, a second set of transmission lines coupled to the horn antenna array for a second polarization orthogonal to the first polarization, and a plurality of L-shaped excitation elements. Each L-shaped excitation element of the plurality of L-shaped excitation elements couples a transmission line from each of the first and second sets of transmission lines to a respective horn antenna of the horn antenna array.

Abstract: A phased array for generating a directed radiation pattern includes a plurality of power divider ports, a first tunable element connected in series between each pair of adjacent power divider ports, an antenna connected to each of the power divider ports, and a second tunable element connected in parallel with each antenna The phased array can include equal phase differences between successive power divider ports, equal amplitude of the signal at each antenna, an equal amount of successive phase change in a signal at each antenna, a source connectible to at least one power divider port including an alternating power supply through a quarter-wave transformer, the first tunable element being either an inductor or a capacitor, the second tunable element being either an inductor or a capacitor, and/or each antenna separated by a successive antenna by a half wavelength.