High-frequency surface acoustic wave device based on thin-film piezoelectric interdigital transducers
Author(s) -
A. K. Sarin Kumar,
Patrycja Paruch,
JeanMarc Triscone,
W. Daniau,
Sylvain Ballandras,
L. Pellegrino,
D. Marré,
Thomas Tybell
Publication year - 2004
Publication title -
applied physics letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.182
H-Index - 442
eISSN - 1077-3118
pISSN - 0003-6951
DOI - 10.1063/1.1787897
Subject(s) - materials science , piezoelectricity , ferroelectricity , polarization (electrochemistry) , transducer , optoelectronics , sputter deposition , thin film , electric field , interdigital transducer , sputtering , optics , acoustics , dielectric , composite material , nanotechnology , physics , chemistry , quantum mechanics
Using high-quality epitaxial c-axis Pb(Zr0.2Ti0.8)O3 films grown by off-axis magnetron sputtering onto metallic (001) Nb-doped SrTiO3 substrates, a nonconventional thin-film surface acoustic wave device based on periodic piezoelectric transducers was realized. The piezoelectric transducers consist of a series of ferroelectric domains with alternating polarization states. The artificial modification of the ferroelectric domain structure is performed by using an atomic force microscope tip as a source of electric field, allowing local switching of the polarization. Devices with 1.2 and 0.8μm wavelength, defined by the modulation period of the polarization, and corresponding to central frequencies in the range 1.50–3.50GHz have been realized and tested.Using high-quality epitaxial c-axis Pb(Zr0.2Ti0.8)O3 films grown by off-axis magnetron sputtering onto metallic (001) Nb-doped SrTiO3 substrates, a nonconventional thin-film surface acoustic wave device based on periodic piezoelectric transducers was realized. The piezoelectric transducers consist of a series of ferroelectric domains with alternating polarization states. The artificial modification of the ferroelectric domain structure is performed by using an atomic force microscope tip as a source of electric field, allowing local switching of the polarization. Devices with 1.2 and 0.8μm wavelength, defined by the modulation period of the polarization, and corresponding to central frequencies in the range 1.50–3.50GHz have been realized and tested.
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