Electroacoustic resonator, filter, duplexer and method for determining parameters of a resonator
AssigneeEpcos AG
InventorEdgar Schmidhammer
Life of this patent
Estimating the term…
Abstract
An electroacoustic resonator includes a resonator area for propagating an acoustic wave and a resonator surface area configured so that, when an input signal power of 0 dBm is applied at a resonant frequency fr, power density in the resonator area does not exceed 40 dBm/m2. An electroacoustic resonator includes a resonator surface area configured so that a critical input signal power PIIPn at an nth-order intercept point IPn is at least 80 dBm for n=2 and/or 80 dBm for n=3.
Claims39
An electroacoustic resonator comprising:
- a resonator surface area configured so that a critical input signal power at an nth-order intercept point IPn is at least 80 dBm for n =2 and/or at least 50 dBm for n =3.
An electroacoustic resonator comprising:
- a resonator area for propagating an acoustic wave;
- and
- a resonator surface area configured so that, when an input signal power of 0 dBm is applied at a resonant frequency fr, power density in the resonator area does not exceed 40 dBm/m2.
An electroacoustic resonator comprising:
- a resonator area for propagating an acoustic wave;
- and
- a resonator surface area configured so that, when an input signal power of 0 dBm is applied at a resonant frequency fr, power density in the resonator area does not exceed 55 dBm/m2.
An electroacoustic resonator comprising:
- a resonator area for propagating an acoustic wave;
- and
- a resonator surface area configured so that, when an input signal power of 0 dBm is applied at a resonant frequency fr, power density in the resonator area does not exceed 70 dBm/m2.
A method comprising:
- obtaining a signal at a resonator;
- determining transmission characteristic curves of the resonator based on the obtained signal, the resonator having a resonator surface area for a fundamental mode and an nth-order spectral component generated in the resonator, where n is a whole number of at least two and the nth-order spectral component is selected from an nth-order harmonic and/or an nth-order intermodulation product, wherein, in the resonator, output signal power is determined as a function of input signal power;
- determining an intersection point of linearly extrapolated linear ranges of the transmission characteristic curves;
- determining an actual critical input signal power of the resonator based on the intersection point;
- comparing the actual critical input signal power to a predetermined target level for a critical input signal power;
- varying resonator surface area if there is a deviation of the actual critical input signal power from the predetermined target level;
- determining values of the actual critical input signal power for a series of resonator surface areas obtained by the varying;
- and
- determining a minimum value for the resonator surface area at which the actual critical input signal power of the resonator achieves the predetermined target level based on the values of the actual critical input signal power for the series of resonator surface areas.
A method comprising:
- obtaining a signal at a resonator;
- determining transmission characteristic curves of the resonator based on the obtained signal, the resonator having a resonator surface area for a fundamental mode and an nth-order spectral component generated in the resonator, where n is a whole number of at least two and the nth-order spectral component is selected from an nth-order harmonic and/or an nth-order intermodulation product, wherein output signal power of the resonator is determined as a function of input signal power of the resonator;
- determining an intersection point of linearly extrapolated linear ranges of the transmission characteristic curves;
- determining an actual critical output signal power of the resonator based on the intersection point;
- comparing the actual critical output signal power to a predetermined target level for a critical output signal power;
- varying the resonator surface area if there is a deviation of the actual critical output signal power from the predetermined target level;
- determining values of the actual critical output signal power for a series of resonator surface areas obtained by the varying;
- and
- determining a minimum value for the resonator surface area at which the actual critical input signal power of the resonator achieves the predetermined target level based on the values of the actual critical output signal power for the series of resonator surface areas.
A method performed using a resonator that is a bulk acoustic wave resonator, the method comprising:
- obtaining a signal at the resonator;
- determining transmission characteristic curves of the resonator based on the obtained signal, the resonator having a layer of thickness of a piezoelectric layer for a fundamental mode and an nth-order spectral component generated in the resonator, where n is a whole number of at least two and the nth-order spectral component is selected from an nth-order harmonic and/or an nth-order intermodulation product, wherein output signal power of the resonator is determined versus input signal power of the resonator;
- determining an intersection point of linearly extrapolated linear ranges of the transmission characteristic curves;
- determining an actual critical input signal power of the resonator corresponding to the intersection point;
- comparing the actual critical input signal power to a predetermined target level for a critical input signal power;
- varying the layer thickness of the piezoelectric layer if there is a deviation of the actual critical input signal power from the predetermined target level;
- determining values of the actual critical input signal power for a series of resonator thicknesses based on the varying;
- and
- determining a minimum value for the layer thickness at which the actual critical input signal power of the resonator achieves the predetermined target level based on values of the actual critical input signal power for a series of resonator thicknesses.
A method for adjusting electrical properties of a resonator operating with bulk acoustic waves, the method comprising:
- reducing a layer thickness of a piezoelectric layer of the resonator;
- selecting a material for at least one electrode of the resonator that has a density that increases a critical input power of the resonator corresponding to an nth-order intercept point.
Dependencies are inferred from the claim text.