Negative Piezoelectric-Based Electric-Field-Actuated Mode-Switchable Multilayer Ferroelectric FBARs for Selective Control of Harmonic Resonances Without Degrading Keff²
Negative Piezoelectric-Based Electric-Field-Actuated Mode-Switchable Multilayer Ferroelectric FBARs for Selective Control of Harmonic Resonances Without Degrading Keff²
复制标题
基于负压电的电场驱动模式可切换多层铁电 FBAR,用于在不降低 Keff² 的情况下选择性控制谐波谐振
DOI:
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发表时间:
2020
期刊:
影响因子:
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通讯作者:
A. Mortazawi
中科院分区:
文献类型:
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作者:
M. Koohi;A. Mortazawi
Mode-switchable ferroelectric thin-film bulk acoustic resonators (FBARs) are presented. Such resonators operate based on a dynamic nonuniform effective piezoelectricity in composite multilayer ferroelectrics with large electrostriction coefficients, like barium strontium titanate (BST). Harmonic resonance modes (<inline-formula> <tex-math notation="LaTeX">$ extit {nf}_{o}$ </tex-math></inline-formula>) of a multilayer ferroelectric bulk acoustic wave (BAW) resonator can be selectively excited with an electromechanical coupling coefficient (<inline-formula> <tex-math notation="LaTeX">${K}_{mathrm {eff}}^{{{2}}}$ </tex-math></inline-formula>) equal to the fundament mode, which is contrary to the trend <inline-formula> <tex-math notation="LaTeX">${K}_{mathrm {eff}}^{{{2}}}propto {1}/{n}^{{{2}}}$ </tex-math></inline-formula> exhibited by conventional piezoelectric BAW resonators. Such a device can selectively be set to resonate at its different resonance harmonics by generating a pattern of nonuniform piezoelectric coefficient proportional to the stress field of each mode with an application of a proper set of dc control voltages applied across the ferroelectric layers. Such a resonator allows for the design of a new class of band-switching filters. As an experimental validation, a mode-switchable FBAR and a band-switching ladder-type filter based on a bilayer ferroelectric BST structure are designed and fabricated for the first time. The bilayer BST FBARs not only can be switched ON or OFF but also by choosing different bias configurations, two resonance modes at 2 and 3.6 GHz can be selectively excited having <inline-formula> <tex-math notation="LaTeX">${K}_{mathrm {eff}}^{{{2}}}$ </tex-math></inline-formula> of 8% and 7%, respectively.