A resonator that includes a substrate with a cavity that extends in a principal surface thereof and a vibrating resonator above the principal surface of the substrate and including bottom and top electrodes with a piezoelectric layer disposed therebetween. Moreover, a silicon dioxide layer is provided above the substrate and below the vibrating resonator to cover the cavity of the substrate, and a silicon layer is provided between the silicon dioxide layer and the vibrating resonator. The bottom electrode, the top electrode and the piezoelectric layer of the vibrating resonator each have a thickness configured to accommodate substantially a half wavelength /2 of the resonator, and the silicon layer has a thickness that accommodates substantially multiple of the half wavelength /2 of the resonator.

A resonator that includes a substrate with a cavity that extends in a principal surface thereof and a vibrating resonator above the principal surface of the substrate and including bottom and top electrodes with a piezoelectric layer disposed therebetween. Moreover, a silicon dioxide layer is provided above the substrate and below the vibrating resonator to cover the cavity of the substrate, and a silicon layer is provided between the silicon dioxide layer and the vibrating resonator. The bottom electrode, the top electrode and the piezoelectric layer of the vibrating resonator each have a thickness configured to accommodate substantially a half wavelength /2 of the resonator, and the silicon layer has a thickness that accommodates substantially multiple of the half wavelength /2 of the resonator.

Acoustic wave devices based on epitaxially grown heterostructures comprising appropriate combinations of epitaxially grown metallic transition metal nitride (TMN) layers, epitaxially grown Group III-nitride (III-N) piezoelectric semiconductor thin film layers, and epitaxially grown perovskite oxide (PO) layers. The devices can include bulk acoustic wave (BAW) devices, surface acoustic wave (SAW) devices, high overtone bulk acoustic resonator (HBAR) devices, and composite devices comprising HBAR devices integrated with high-electron-mobility transistors (HEMTs).

Techniques for improving Bulk Acoustic Wave (BAW) resonator structures are disclosed, including fluidic systems, oscillators and systems that may include such devices. A bulk acoustic wave (BAW) resonator may comprise a substrate and a first layer of piezoelectric material. The bulk acoustic wave (BAW) resonator may comprise a top electrode. A sensing region may be acoustically coupled with the top electrode of the bulk acoustic wave (BAW) resonator.

A family of composite resonator devices having improved performance properties for use in electronic circuits. Each composite device includes two or more resonator electrodes on a single crystal or other resonant material. The two resonators may be connected in series or parallel, based on application requirements. The two resonators have different surface areas or some other type of asymmetry, causing the response of the composite device to have suppressed spurious modes, reduced insertion loss, or both. This is accomplished by designing the electrodes to have different frequency response curves, where the responses can be tuned and combined to reduce undesirable modes. Improvements in acceleration sensitivity and temperature sensitivity are also achieved. Both physically-applied and projected electrode types are disclosed, along with several crystal shapes. The family of composite resonator devices includes both passive and active devices, such as resonators, filters and oscillators.

Techniques for improving acoustic wave device structures are disclosed, including filters, oscillators and systems that may include such devices. First and second layers of piezoelectric material may be acoustically coupled with one another to have a piezoelectrically excitable resonance mode. The first layer of piezoelectric material may have a first piezoelectric axis orientation, and the second layer of piezoelectric material may have a second piezoelectric axis orientation that substantially opposes the first piezoelectric axis orientation of the first layer of piezoelectric material. The first and second layers of piezoelectric material have respective thicknesses so that the acoustic wave device has a resonant frequency that is in a super high frequency band or an extremely high frequency band.

Techniques for improving Bulk Acoustic Wave (BAW) resonator structures are disclosed, including fluidic systems, oscillators and systems that may include such devices. A bulk acoustic wave (BAW) resonator may comprise a substrate and a first layer of piezoelectric material. The bulk acoustic wave (BAW) resonator may comprise a top electrode. A sensing region may be acoustically coupled with the top electrode of the bulk acoustic wave (BAW) resonator.

Techniques for improving Bulk Acoustic Wave (BAW) mass loading of resonator structures are disclosed, including filters, oscillators and systems that may include such devices. First and second layers of piezoelectric material may be acoustically coupled with one another to have a piezoelectrically excitable resonance mode. The first layer of piezoelectric material may have a first piezoelectric axis orientation, and the second layer of piezoelectric material may have a second piezoelectric axis orientation that substantially opposes the first piezoelectric axis orientation of the first layer of piezoelectric material. An acoustic reflector electrode may include a first pair of top metal electrode layers electrically and acoustically coupled with the first and second layer of piezoelectric material to excite the piezoelectrically excitable resonance mode at a resonant frequency of the BAW resonator. The acoustic reflector may include a mass load layer to facilitate a preselected frequency compensation in the resonant frequency.

The present disclosure describes systems and methods for novel phononic frequency combs and related sensing techniques realized by a piezoelectric multimode or single-mode mechanical resonator based on parametric pumping. In one embodiment of such a system, a single frequency electrical input provides an electrical signal comprising an amplitude and a single input frequency to a single-mode mechanical resonator, in which a value of the single input frequency equals twice a value of the resonance mode of the single-mode mechanical resonator. Accordingly, the mechanical resonator is configured to produce at least one phononic frequency comb in response to a motion of the mechanical resonator caused by the electrical signal.

A bulk acoustic wave sensor includes a delay layer. The sensor includes an acoustic mirror and a base resonator. The base resonator includes a piezoelectric layer and two electrodes. One or more delay layers are disposed adjacent to the base resonator. A delay layer may be disposed between the base resonator and the acoustic mirror, a delay layer may be disposed on the base resonator opposite to the acoustic mirror, or both. Each delay section is formed of high quality-factor material. The sensor may define a resonant frequency, and the thickness of each delay section may be an integer multiple of half-wavelengths of the resonant frequency.