20 research outputs found
Anelastic relaxor behavior of Pb(Mg1/3Nb2/3)O3
Elastic storage modulus and loss of relaxor lead magnesium niobate ceramics,
Pb(Mg1/3Nb2/3)O3, have been measured with dynamic mechanical analyzer in single
cantilever mode in the temperature range from 170 K to 320 K and at frequencies
from 0.1 Hz to 50 Hz. The dependence of the elastic susceptibility (inverse
modulus) on temperature and frequency of the driving force has characteristics
of typical relaxor behavior that can be well described with the Vogel-Fulcher
law. The parameters of the Vogel-Fulcher relation exhibit similar values for
the dielectric and anelastic relaxations. Similarities and differences between
anelastic and dielectric relaxor behaviors are identified.Comment: accepted in Applied Physics Letter
Effect of thermal annealing on dielectric and ferroelectric properties of aerosol-deposited thick films
In this work, the effects of thermal annealing at 500 {\deg}C on
aerosol-deposited
thick films on stainless-steel substrates are investigated using two
complementary methods at high and low applied external electric fields. The
first one is Positive Up Negative Down method, which allows us to obtain
information about the switching and non-switching contributions to the
polarization. It shows that the as-deposited film is ferroelectric before
annealing, since it has a switching contribution to the polarization. After
annealing, both the switching and non-switching contributions to polarization
increased by a factor of 1.6 and 2.33, respectively, indicating stronger
ferroelectric behavior. The second method is based on impedance spectroscopy
coupled with Rayleigh analysis. The results show that post-deposition thermal
annealing increases the reversible domain wall contribution to the dielectric
permittivity by a factor 11 while keeping the threshold field similar. This
indicates, after annealing, domain wall density is larger while domain wall
mobility remains similar. These two complementary characterization methods show
that annealing increases the ferroelectric behavior of the thick film by
increasing the domain wall density and its influence is visible both on
polarization versus electric field loop and dielectric permittivity
Magnetoelectric coupling in multiferroic CFO/BCTSn core shell nanofibers elaborated by co-axial electrospinning method
Multiferroic CoFe2O4-Ba0.95Ca0.05Ti0.89Sn0.11O3 core-shell nanofibers
(CFO@BCTSn NFs) were synthesized by a sol-gel co-axial electrospinning
technique. The scanning electron microscope and transmission electron
microscope were used to check nanofibers' core-shell structure/configuration.
X-ray diffraction and a high-resolution transmission electron microscope were
used to confirm the spinel structure of CFO and the perovskite structure of
BCTSn. The magnetic character of the resultant CFO@BCTSn NFs was determined by
SQUID magnetometry. The piezoelectricity was verified using piezo-response
force microscopy, which revealed an entirely covered ferroelectric shell
outline, in accordance with SEM and TEM observations. The magnetoelectric (ME)
coefficient was measured as a function of the applied external DC magnetic
field. The maximum ME coefficient obtained for the CFO@BCTSn NFs was 346 mV
cm-1 Oe-1. The high magnetoelectric coupling suggests that CFO@BCTSn NFs could
be a promising candidate for magnetic field sensor and magnetoelectric device
applications
Effects of strontium doping on microstructure and functional properties of solution-derived potassium sodium niobate thin films
The effects of strontium doping (0-2 mol%) on structure, microstructure and functional properties of potassium sodium niobate (KNN) thin films deposited on Pt(111)/TiOy/SiO2/Si substrates were investigated. Incorporation of Sr up to 1 mol% into the KNN crystal lattice hindered the grain growth, vertical roughness and contributed to the fine-grained and dense thin film microstructure with monoclinic crystal syngony. This effectively reduced leakage current and improved ferroelectric characteristics. Higher doping content (2 mol%) led to the formation of secondary phases and complete deterioration of functional properties. Stabilization of 1 mol% Sr-doped KNN solution with diethanolamine resulted in the film with dielectric constant and losses of 394 and 0.018 at 100 kHz, respectively, leakage current of 3.8 . 10(-8) A/cm(2) at 100 kV/cm and well saturated ferroelectric hysteresis with P-r of 6.8 mu C/cm(2) and low E-c of 85 kV/cm. Benefiting from improved leakage current characteristics at high electric fields and less defect structure, the film showed maximal local piezoelectric coefficient, d(33) similar to 110 pm/V determined by piezo-response force microscopy (PFM), ability to reach fully saturated local hysteresis under low switching DC voltage of 15 V and good ferroelectric domain mobility proven by successful in-situ poling of chosen area using PFM lithography
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>
A complex domain structure with variations in the morphology is observed at ambient temperature in monoclinic Pb(Fe1/2Nb1/2)O3. Using electron microscopy and piezoresponse force microscopy, it is possible to reveal micrometre-sized wedge, lamellar-like, and irregularly shaped domains. By increasing the temperature, the domain structure persists up to 80 °C, and then starts to disappear at around 100 °C due to the proximity of the ferroelectric–paraelectric phase transition, in agreement with macroscopic dielectric measurements. In order to understand to what degree domain switching can occur in the ceramic, the mobility of the domain walls was studied at ambient temperature. The in situ poling experiment performed using piezoresponse force microscopy resulted in an almost perfectly poled area, providing evidence that all types of domains can be easily switched. By poling half an area with 20 V and the other half with −20 V, two domains separated by a straight domain wall were created, indicating that Pb(Fe1/2Nb1/2)O3 is a promising material for domain-wall engineering
0.65Pb(Mg 1/3 Nb 2/3 )O 3 –0.35PbTiO 3 Thick Films for High-Frequency Piezoelectric Transducer Applications
International audienceThe properties of 0.65Pb(Mg 1/3 Nb 2/3 )O 3 –0.35PbTiO 3 (0.65PMN–0.35PT) thick films were studiedfor high-frequency piezoelectric transducer applications. The films were prepared by screen-printinga thick-film paste on platinized alumina substrates and subsequent sintering at 950 °C. Theeffective thickness-coupling factor of these films was close to 48%, which is comparable with bulkceramics having the same compositions. Furthermore, simulations of two configurations representingone element of a high-frequency linear-array transducer (30 MHz) suggests that 0.65PMN–0.35PTthick-films in 50 Ω electrical matching environment improves the performance in comparison withstandard Pb(Zr,Ti)O 3 (PZT) compositions
Structural and electrical properties of 0.57PSN-0.43PT ceramics prepared by mechanochemical synthesis and sintered at low temperature
International audienceIn this investigation we show that the dielectric, ferroelectric and piezoelectric properties of stoichiometric 0.57Pb(Sc1/2Nb1/2)O3-0.43PbTiO3 (0.57PSN-0.43PT) ceramics prepared by mechanochemical synthesis are comparable or even better than the properties of 0.57PSN-0.43PT ceramics with Nb doping, which was proposed to enhance the electrical properties. Here, the stoichiometric ceramic was sintered to 97% of theoretical density at a temperature of 1000 ◦C, which is 200-300 ◦C lower than previously reported. The dielectric constant ε, remnant polarization Pr, piezoelectric coefficient d33, coupling coefficients kp and kt and mechanical quality factor Qm of the ceramics prepared by mechanochemical synthesis were 2200, 43 C/cm2, 570 pC/N, 0.71, 0.56 and 38, respectively. The effects of the poling field on the structural and electrical properties of the 0.57PSN-0.43PT ceramics were investigated. The results show that the ratio of the monoclinic to the tetragonal phases is influenced by the application of the poling electric field. The non-poled ceramics contain 71% of the monoclinic phase and 29% of the tetragonal phase. The highest d33, kp and kt were measured for ceramics poled at an electric field of 3 kV/mm. For these poled ceramics a phase determination of 86% monoclinic phase and 14% tetragonal phase was obtained from Rietveld refinements. © 2011 Elsevie
Effect of thermal annealing on dielectric and ferroelectric properties of aerosol-deposited 0.65Pb(Mg1/3Nb2/3)O3-0.35 PbTiO3 thick films
International audienceIn this work, the effects of thermal annealing at 500°C on aerosol-deposited 0.65Pb(Mg1/3Nb2/3)O 3-0.35PbTiO 3 thick films on stainless-steel substrates are investigated using two complementary methods at high and low applied external electric fields. The first one is Positive Up Negative Down method, which allows us to obtain information about the switching and non-switching contributions to the polarization. It shows that the as-deposited film is ferroelectric before annealing, since it has a switching contribution to the polarization. After annealing, both the switching and non-switching contributions to polarization increased by a factor of 1.6 and 2.33, respectively, indicating stronger ferroelectric behavior. The second method is based on impedance spectroscopy coupled with Rayleigh analysis. The results show that post-deposition thermal annealing increases the reversible domain wall contribution to the dielectric permittivity by a factor 11 while keeping the threshold field similar. This indicates, after annealing, domain wall density is larger while domain wall mobility remains similar. These two complementary characterization methods show that annealing increases the ferroelectric behavior of the thick film by increasing the domain wall density and its influence is visible both on polarization versus electric field loop and dielectric permittivity