Thickness‐Dependent Properties of Relaxor‐PbTiO3 Ferroelectrics for Ultrasonic Transducers

The electrical properties of Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) (PMN-PT) based polycrystalline ceramics and single crystals were investigated as a function of scale ranging from 500 microns to 30 microns. Fine-grained PMN-PT ceramics exhibited comparable dielectric and piezoelectric properties to their coarse-grained counterpart in the low frequency range (<10 MHz), but offered greater mechanical strength and improved property stability with decreasing thickness, corresponding to higher operating frequencies (>40 MHz). For PMN-PT single crystals, however, the dielectric and electromechanical properties degraded with decreasing thickness, while ternary Pb(In(1/2)Nb(1/2))O(3)-Pb(Mg(1/3)Nb(2/3))O(3)-PbTiO(3) (PIN-PMN-PT) exhibited minimal size dependent behavior. The origin of property degradation of PMN-PT crystals was further studied by investigating the dielectric permittivity at high temperatures, and domain observations using optical polarized light microscopy. The results demonstrated that the thickness dependent properties of relaxor-PT ferroelectrics are closely related to the domain size with respect to the associated macroscopic scale of the samples.

[1]  Wenwu Cao,et al.  Electromechanical properties of fine-grain, 0.7 Pb(Mg/sub 1/3/Nb/sub 2/3/)O/sub 3/-0.3PbTiO/sub 3/ ceramics , 2004, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[2]  Matthew J. Davis,et al.  Rotator and extender ferroelectrics: Importance of the shear coefficient to the piezoelectric properties of domain-engineered crystals and ceramics , 2007, cond-mat/0703121.

[3]  Field-induced piezoelectric response in Pb(Mg1/3Nb2/3)O3-PbTiO3 single crystals , 2006 .

[4]  Thomas R. Shrout,et al.  Effect of grain size on actuator properties of piezoelectric ceramics , 1998, Smart Structures.

[5]  R. Whatmore,et al.  The effect of grinding conditions on lead zirconate titanate machinability , 1999 .

[6]  S. Jyomura,et al.  Effects of the lapped surface layers on the dielectric properties of ferroelectric ceramics , 1980 .

[7]  I. Lloyd,et al.  Modification of surface texture by grinding and polishing lead zirconate titanate ceramics , 1992 .

[8]  E. W. Jacobs,et al.  In situ x-ray diffraction study of an electric field induced phase transition in the single crystal relaxor ferroelectric, 92% Pb(Zn1/3Nb2/3)O3–8% PbTiO3 , 1999 .

[9]  E. C. Subbarao,et al.  Domain Effects in Polycrystalline Barium Titanate , 1957 .

[10]  Kenji Uchino,et al.  Dielectric and Piezoelectric Properties of 0.91Pb(Zn1/3Nb2/3)O3-0.09PbTiO3 Single Crystals , 1982 .

[11]  Clive A. Randall,et al.  Grain size and domain size relations in bulk ceramic ferroelectric materials , 1996 .

[12]  Helmut Ermert,et al.  In vivo ultrasound biomicroscopy , 1993 .

[13]  Dragan Damjanovic Comments on Origins of Enhanced Piezoelectric Properties in Ferroelectrics , 2009, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[14]  Thomas R. Shrout,et al.  Characterization of Pb(In1/2Nb1/2)O3–Pb(Mg1/3Nb2/3)O3–PbTiO3 ferroelectric crystal with enhanced phase transition temperatures , 2008 .

[15]  F. J. Kumar,et al.  Trapped metastable phases in Pb(Zn1/3Nb2/3)O3-(8-9)%PbTiO3 single-crystal wafers , 2003 .

[16]  T. Shrout,et al.  Ultrahigh strain and piezoelectric behavior in relaxor based ferroelectric single crystals , 1997 .

[17]  Xiaoning Jiang,et al.  Piezoelectric transducers using micromachined bulk piezo substrates , 2008, 2008 IEEE Sensors.

[18]  Ronald E. Cohen,et al.  Polarization rotation mechanism for ultrahigh electromechanical response in single-crystal piezoelectrics , 2000, Nature.

[19]  Thomas R. Shrout,et al.  Electromechanical characterization of [Formula: see text] crystals as a function of crystallographic orientation and temperature. , 2009, Journal of applied physics.

[20]  L. Wang,et al.  A compliance/stiffness matrix formulation of general Green's function and effective permittivity for piezoelectric multilayers , 2004, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[21]  F. S. Foster,et al.  Beyond 30 MHz [applications of high-frequency ultrasound imaging] , 1996 .

[22]  Xuecang Geng,et al.  Single crystal piezoelectric composite transducers for ultrasound NDE applications , 2008, SPIE Smart Structures and Materials + Nondestructive Evaluation and Health Monitoring.

[23]  F. Foster,et al.  Characterization of lead zirconate titanate ceramics for use in miniature high-frequency (20-80 MHz) transducers , 1991, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[24]  G. Arlt,et al.  Dielectric properties of fine‐grained barium titanate ceramics , 1985 .

[25]  A. Virkar,et al.  Fracture Mechanisms in Ferroelectric‐Ferroelastic Lead Zirconate Titanate (Zr: Ti=0.54:0.46) Ceramics , 1990 .

[26]  W. A. Smith,et al.  New opportunities in ultrasonic transducers emerging from innovations in piezoelectric materials (Invited Paper) , 1992, SPIE Optics + Photonics.

[27]  K. Shung,et al.  Piezoceramics for high-frequency (20 to 100 MHz) single-element imaging transducers , 1997 .

[28]  Qifa Zhou,et al.  Piezoelectric materials for high frequency medical imaging applications: A review , 2007 .