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Bias controlled electrostrictive longitudinal resonance in X-cut lithium niobate thin films resonator
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10.1063/1.3598410
/content/aip/journal/apl/98/23/10.1063/1.3598410
http://aip.metastore.ingenta.com/content/aip/journal/apl/98/23/10.1063/1.3598410
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Figures

Image of FIG. 1.
FIG. 1.

(a) Experimental and models of the real part of the impedance of the HBAR device with 175 V bias superimposed to the RF signal presented in a large frequency range. “Model shear” and “model longi” take into account, respectively, the piezoelectric fast shear (FS) wave alone and the electrostrictive (E) longitudinal wave alone. For sake of clarity, model only fits the average of the curve and not all HBAR peaks. Inset: schematic of the cross section of the HBAR resonator. (b) Experimental of the real part of the impedance of the resonator vs frequency at 0 and 175 V bias presented in a narrow frequency range between 2.47 and 2.50 GHz (FS, SS, and E wave).

Image of FIG. 2.
FIG. 2.

Amplitude of the real parts of impedance (ReZ) and admittance (ReY) of the E longitudinal wave generated in LNO HBAR by 175 V bias. Each point represents the difference between one E-HBAR peak and the floor value. The Mason model used is fitted by adjusting only the electromechanical coupling.

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/content/aip/journal/apl/98/23/10.1063/1.3598410
2011-06-09
2014-04-25
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Bias controlled electrostrictive longitudinal resonance in X-cut lithium niobate thin films resonator
http://aip.metastore.ingenta.com/content/aip/journal/apl/98/23/10.1063/1.3598410
10.1063/1.3598410
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