“…6 7 -(Sm 0.12 Bi 0.88 FeO 3 )−0.33BaTiO 3 ceramics. 9 Moreover, a BF−BT solid solution has a temperatureindependent morphotropic phase boundary (MPB) when the fraction of BT is between 0.25 and 0.4, which extends the research interests beyond the realm of ferromagnetic and ferroelectricity. 10−14 Benefiting from the abundant phase and domain structures, improvements in piezoelectricity were usually observed near the MPB.…”
Section: Introductionmentioning
confidence: 91%
“…As a result, an ultrahigh energy density of ∼152 J/cm 3 with high efficiency of about >90% is realized in the latter system, which is among the highest values for reported dielectric materials. The initial research surge in BFO was driven by its single-phase multiferroic character at room temperature, so many researchers also predicted and confirmed the ferromagnetic properties in the BF–BT system. − For example, the destabilized cycloidal spin structure resulting from the distortion of FeO 6 octahedra, gives rise to a remanent magnetization of ∼0.55 emu/g and magnetoelectric coupling coefficients of ∼5 mV/(cm·Oe) in the 0.67(Sm 0.12 Bi 0.88 FeO 3 )–0.33BaTiO 3 ceramics …”
Ferroelectric solid solutions with composition near the morphotropic phase boundary (MPB) have gained extensive attention recently due to their excellent ferroelectric and piezoelectric properties. Here, we have demonstrated a strategy to realize the controllable preparation of BiFeO 3 −BaTiO 3 (BF−BT) epitaxial films near the MPB. A series of high-quality BF−BT films were fabricated by pulsed laser deposition via adjusting oxygen partial pressure (PO 2 ) using a BF−BT ceramic target. A continuous transition from rhombohedral to tetragonal phase was observed upon increasing PO 2 . Particularly, the film with a pure tetragonal phase exhibited a large remnant polarization of ∼90.6 μC/cm 2 , while excellent piezoelectric performance with an ultrahigh strain (∼0.48%) was obtained in the film with coexisting rhombohedral and tetragonal phases. The excellent ferroelectric and piezoelectric properties endow the BF−BT system near the MPB with great application prospects in lead-free electronic devices.
“…6 7 -(Sm 0.12 Bi 0.88 FeO 3 )−0.33BaTiO 3 ceramics. 9 Moreover, a BF−BT solid solution has a temperatureindependent morphotropic phase boundary (MPB) when the fraction of BT is between 0.25 and 0.4, which extends the research interests beyond the realm of ferromagnetic and ferroelectricity. 10−14 Benefiting from the abundant phase and domain structures, improvements in piezoelectricity were usually observed near the MPB.…”
Section: Introductionmentioning
confidence: 91%
“…As a result, an ultrahigh energy density of ∼152 J/cm 3 with high efficiency of about >90% is realized in the latter system, which is among the highest values for reported dielectric materials. The initial research surge in BFO was driven by its single-phase multiferroic character at room temperature, so many researchers also predicted and confirmed the ferromagnetic properties in the BF–BT system. − For example, the destabilized cycloidal spin structure resulting from the distortion of FeO 6 octahedra, gives rise to a remanent magnetization of ∼0.55 emu/g and magnetoelectric coupling coefficients of ∼5 mV/(cm·Oe) in the 0.67(Sm 0.12 Bi 0.88 FeO 3 )–0.33BaTiO 3 ceramics …”
Ferroelectric solid solutions with composition near the morphotropic phase boundary (MPB) have gained extensive attention recently due to their excellent ferroelectric and piezoelectric properties. Here, we have demonstrated a strategy to realize the controllable preparation of BiFeO 3 −BaTiO 3 (BF−BT) epitaxial films near the MPB. A series of high-quality BF−BT films were fabricated by pulsed laser deposition via adjusting oxygen partial pressure (PO 2 ) using a BF−BT ceramic target. A continuous transition from rhombohedral to tetragonal phase was observed upon increasing PO 2 . Particularly, the film with a pure tetragonal phase exhibited a large remnant polarization of ∼90.6 μC/cm 2 , while excellent piezoelectric performance with an ultrahigh strain (∼0.48%) was obtained in the film with coexisting rhombohedral and tetragonal phases. The excellent ferroelectric and piezoelectric properties endow the BF−BT system near the MPB with great application prospects in lead-free electronic devices.
“…The destabilized degree in spin structure caused by sintering temperature influences the magnetoelectric coefficient. 162 The cerium-modified BTO− BFO ceramics have heightened the magnetic properties. The reason for the great magnetism was the Ce 3+ /Ce 4+ induced suppression of spin chains and grain growth function.…”
Section: Sangwook Kim Et Al Supported the Xbto−(1−x)bfomentioning
confidence: 99%
“…In this system, the origin of the magnetoelectric coupling effect is due to the destabilization in the cycloidal form, which results in the distortion of the FeO 6 octahedral. The destabilized degree in spin structure caused by sintering temperature influences the magnetoelectric coefficient . The cerium-modified BTO–BFO ceramics have heightened the magnetic properties.…”
Barium
titanate (BaTiO3) and Bismuth ferrite (BiFeO3) have been investigated for many years. Both of them have
good electrical properties in the application of industries such as
flexible displays, actuators, transducers, flexible memory, multilayer
ceramic capacitors, etc. Moreover, BiFeO3 is a room temperature
multiferroic material that adds a halo to it. Although there are some
shortcomings compared with some properties of lead-based ceramics,
environmental friendly materials will be the future trend. The solid
solution of BaTiO3 and BiFeO3 exactly meets
this requirement. There are many reports related to it, but there
are few systemic articles focused on it. So, this review recalls the
progress of binary ferroelectric material: BaTiO3–BiFeO3 ceramic, especially in the field of ferroelectric, piezoelectric,
energy-storage properties. Furthermore, the preparation approaches
to functional ceramics are also illustrated here. Finally, we deliver
a summary of this material.
“…Nevertheless, attention should be paid to octahedra distortion in the perovskite structure. Li et al reported that the variation in distortion degree of oxygen octahedra contributing to the optimization of multiferroic properties 12 . Moreover due to the influence of the second‐order Jahn‐Teller (SOJT) concept, the displacement of the cation center results in asymmetric bonding configurations and forms uniform polarization directions 13 .…”
Here, B‐site doped 0.725BiFe0.98M0.02O3‐0.275BaTiO3 (M = Fe, Sc, Ga, and Al) + 0.8 mol% MnO2 (abbreviated as BF, BS, BG, and BA) (BFM‐BT) ceramics were designed and prepared to modulate octahedral distortions. According to bond‐valence calculations based on XRD Rietveld refinement data, B‐site doped BFM‐BT ceramics tended to have a higher distortion as the radius of the doping ion decreases, and obtained a great improvement of ferroelectric and piezoelectric performances. B‐site‐doped BFM‐BT ceramics significantly inhibited the formation of impurities, leading to better ferroelectric and piezoelectric performances. The BFM‐BT ceramics exhibited high Curie temperature of 519‐530℃ and good temperature stability for piezoelectric performances. The d33 values of BF, BS, and BA ceramics remained the room temperature value ranging from room temperature to 470℃. Meanwhile the content of impure phases, oxygen vacancies and valence of Fe3+ to Fe2+ decreased with the decreasing radii of B‐site doping ions.
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