Raised-Frame BAW Resonators for Low Lateral Energy Leakage
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Solution Overview
Problem
Existing bulk acoustic wave (BAW) devices face challenges in achieving high quality factor (Q) and low insertion loss, particularly due to lateral energy leakage and spurious modes that affect performance in carrier aggregation bands.
Innovation Solution
The introduction of a raised frame structure with a low acoustic impedance material, such as silicon dioxide, between electrodes and a piezoelectric layer, combined with a higher impedance material, effectively reduces lateral energy leakage and spurious modes by configuring the frame structure to be outside the carrier aggregation bands, thereby enhancing the quality factor (Q) and reducing Gamma loss.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If a raised frame structure with low acoustic impedance material is introduced, then lateral energy leakage is reduced and quality factor is improved, but device complexity increases
Solution Approach 1:
The device is segmented into distinct functional regions: an active region for acoustic wave generation and a raised frame region for acoustic confinement. This segmentation allows the raised frame structure to independently address lateral energy leakage without interfering with the core resonator function, thereby improving quality factor while maintaining clear functional separation.
Solution Approach 2:
A raised frame structure composed of low acoustic impedance material (such as silicon dioxide) is introduced as an intermediary element between the active region and the substrate. This intermediary structure acts as an acoustic barrier that reduces lateral energy leakage into the substrate, thereby improving the quality factor without requiring fundamental changes to the resonator design.
2Loss of energy
If the raised frame structure is positioned outside the carrier aggregation bands, then spurious modes are reduced and insertion loss is minimized, but the frequency tuning range is constrained
Solution Approach 1:
The raised frame structure is positioned at specific locations outside the carrier aggregation bands where spurious modes typically occur. By locally addressing these problematic frequency regions rather than attempting global frequency tuning, the structure minimizes insertion loss at critical operating frequencies while maintaining adaptability for different carrier aggregation configurations.
Solution Approach 2:
The acoustic impedance parameters of the raised frame structure are specifically optimized to create acoustic barriers at frequencies outside the carrier aggregation bands. By controlling the impedance contrast between the raised frame material and the surrounding structures, the design suppresses spurious modes and reduces insertion loss while allowing the resonator to operate across desired frequency ranges.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
The raised frame structure achieves low insertion loss and high Q factors, improving the performance of BAW devices by minimizing lateral energy leakage and spurious modes, particularly in carrier aggregation applications.
Implementation Method 1
A raised frame structure can include a first raised frame layer and a second raised frame layer. The second raised frame layer can have a higher acoustic impedance than the first raised frame layer.
Implementation Method 2
a piezoelectric layer between the first electrode and the second electrode
Data Source
AI summary
Aspects of this disclosure relate to bulk acoustic wave devices that have a raised frame structure. The raised frame structure can include a first raised frame layer that has a relatively low acoustic impedance. The raised frame structure can include a second raised frame layer that has a relatively high acoustic impedance. The first raised frame layer can have a thickness that is between about 0.02 and about 0.4 times the combined thickness H of the bulk acoustic wave device. The first raised frame layer can have a thickness that is between about 0.01 and about 0.2 times the resonant wavelength λ of the bulk acoustic wave device.


