Precursor dynamics of a cubic to tetragonal ferroelectric phase transition in BaTiO3 is studied by the accurate measurement of the second harmonic generation (SHG) integral intensities. A finite signal holds for the SHG integrated intensity above the ferroelectric Curie temperature Tc=403 K. Above the Burn’s temperature Td≈580 K, the power law with the exponent γ=1 shows normal SHG nature originating from the hyper-Raman scattering by dynamical polar excitations, while, below Td, a SHG signal from polar nanoregions becomes dominant with the larger exponent γ=2. Such a crossover of the power law exponent near Td is discussed on the basis of the effective Hamiltonian method and Monte Carlo simulation
The infrared properties of a system of first-order-coupled phonons are analyzed. The dielectric func...
The three-dimensional distribution of the x-ray diffuse scattering intensity of BaTiO 3 has been rec...
The broadband gigahertz dynamics of a relaxor ferroelectric crystal 0.70Pb(Sc1/2Nb1/2)O3-0.30PbTiO3 ...
The nature of precursor phenomena in the paraelectric phase of ferroelectrics is one of the main qu...
The dynamic properties of elastic domain walls in BaTiO3 were investigated using resonance ultrasoni...
BaTiO3 appears in cubic and hexagonal variants, both of which are centrosymmetric. Samples of cubic ...
Whereas low-temperature ferroelectrics have a well understood ordered spatial dipole arrangement, th...
By using a symmetry motivated basis to evaluate local distortions against pair distribution function...
For tetragonal phase of BaTiO3 in framework of vibronic theory of ferroelectricity components and ...
We calculate the effects of conduction band electrons (CBEs), introduced by doping or photoexcitatio...
Nanocrystalline powders of 1% Yb$^{3+}$-doped BaTiO$_{3}$ sintered at different temperatures were ob...
An experimental method, Resonant Piezoelectric Spectroscopy (RPS), is introduced for the detection o...
Using quantum mechanics (QM, Density Functional Theory) we show that all four phases of barium titan...
We report the synthesis, structural and ferroelectric characterization of continuous well-aligned na...
The local structure of high-pressure BaTiO3 has been interrogated by neutron total scattering method...
The infrared properties of a system of first-order-coupled phonons are analyzed. The dielectric func...
The three-dimensional distribution of the x-ray diffuse scattering intensity of BaTiO 3 has been rec...
The broadband gigahertz dynamics of a relaxor ferroelectric crystal 0.70Pb(Sc1/2Nb1/2)O3-0.30PbTiO3 ...
The nature of precursor phenomena in the paraelectric phase of ferroelectrics is one of the main qu...
The dynamic properties of elastic domain walls in BaTiO3 were investigated using resonance ultrasoni...
BaTiO3 appears in cubic and hexagonal variants, both of which are centrosymmetric. Samples of cubic ...
Whereas low-temperature ferroelectrics have a well understood ordered spatial dipole arrangement, th...
By using a symmetry motivated basis to evaluate local distortions against pair distribution function...
For tetragonal phase of BaTiO3 in framework of vibronic theory of ferroelectricity components and ...
We calculate the effects of conduction band electrons (CBEs), introduced by doping or photoexcitatio...
Nanocrystalline powders of 1% Yb$^{3+}$-doped BaTiO$_{3}$ sintered at different temperatures were ob...
An experimental method, Resonant Piezoelectric Spectroscopy (RPS), is introduced for the detection o...
Using quantum mechanics (QM, Density Functional Theory) we show that all four phases of barium titan...
We report the synthesis, structural and ferroelectric characterization of continuous well-aligned na...
The local structure of high-pressure BaTiO3 has been interrogated by neutron total scattering method...
The infrared properties of a system of first-order-coupled phonons are analyzed. The dielectric func...
The three-dimensional distribution of the x-ray diffuse scattering intensity of BaTiO 3 has been rec...
The broadband gigahertz dynamics of a relaxor ferroelectric crystal 0.70Pb(Sc1/2Nb1/2)O3-0.30PbTiO3 ...