Abstract:The phonon spectra of calcium, strontium, barium, radium, cadmium, zinc, magnesium, germanium, tin, and lead titanates with the perovskite structure are calculated from first principles within the density functional theory. By analyzing the unstable modes in the phonon spectra, the possible lattice distortions are determined and the energies of the corresponding phases are calculated. From analyzing the phonon spectra, force constants, and eigenvectors of TO phonons, a conclusion is drawn on the origin of the … Show more
“…This means that the formation of the monoclinic phase with P b space group and tilted polarization vector is energetically unfavorable. The calculation using the formula (1) shows that the energy minima are observed at the mode amplitudes of (ξ = 0.03332, η = 0) and (ξ = 0, η = 0.02288) and that the energy gains associated with these lattice distortions are 6.16 and 1.86 meV, respectively. They are close to the corresponding energy gains of the true distortions (see Sec.…”
Section: Fig 3 Relative Contributions Of Different Modes With B1umentioning
confidence: 99%
“…1 have revealed that orthorhombic phases of CdTiO 3 , ZnTiO 3 , and MgTiO 3 with the P bnm structure exhibit the ferroelectric instability which appears in their phonon spectra as one or two unstable modes with symmetries B 1u and B 2u at the Γ point. In this work, the characteristics of these modes are considered and the results of first-principles calculations of the crystal structure, phonon spectra, and spontaneous polarization of the parent orthorhombic CdTiO 3 phase with P bnm structure and its two ferroelectrically distorted orthorhombic modifications (with P bn2 1 and P b2 1 m space groups) are compared with available experimental data.…”
Section: Introductionmentioning
confidence: 99%
“…Here, ν = −2a/M * /2π is the value of an imaginary mode frequency in the high-symmetry configuration (maximum of the potential barrier) determined in the classical (BornOppenheimer) approximation, and E 0 = a 2 /4b is the depth of the potential well for the V (x) potential. For the four-minimum potential well described by equation (1), the quantitative value of the criterion can be slightly different.…”
The crystal structures and phonon spectra of orthorhombic cadmium titanate with the P bnm structure and of its two possible ferroelectrically distorted phases with P bn21 and P b21m space groups were calculated from first principles within the density functional theory. The obtained structural parameters and frequencies of Raman-and infrared-active modes are in good agreement with available experimental data for the P bnm phase. Expansion of the total energy in a Taylor series of two order parameters showed that the ground state of the system corresponds to the P bn21 structure into which the P bnm phase transforms through a second-order phase transition without intermediate phases. A substantial discrepancy between the calculated and experimentally observed lattice distortions and spontaneous polarization in the polar phase was explained by quantum fluctuations as well as by existence of twinning and competing long-period structures.
“…This means that the formation of the monoclinic phase with P b space group and tilted polarization vector is energetically unfavorable. The calculation using the formula (1) shows that the energy minima are observed at the mode amplitudes of (ξ = 0.03332, η = 0) and (ξ = 0, η = 0.02288) and that the energy gains associated with these lattice distortions are 6.16 and 1.86 meV, respectively. They are close to the corresponding energy gains of the true distortions (see Sec.…”
Section: Fig 3 Relative Contributions Of Different Modes With B1umentioning
confidence: 99%
“…1 have revealed that orthorhombic phases of CdTiO 3 , ZnTiO 3 , and MgTiO 3 with the P bnm structure exhibit the ferroelectric instability which appears in their phonon spectra as one or two unstable modes with symmetries B 1u and B 2u at the Γ point. In this work, the characteristics of these modes are considered and the results of first-principles calculations of the crystal structure, phonon spectra, and spontaneous polarization of the parent orthorhombic CdTiO 3 phase with P bnm structure and its two ferroelectrically distorted orthorhombic modifications (with P bn2 1 and P b2 1 m space groups) are compared with available experimental data.…”
Section: Introductionmentioning
confidence: 99%
“…Here, ν = −2a/M * /2π is the value of an imaginary mode frequency in the high-symmetry configuration (maximum of the potential barrier) determined in the classical (BornOppenheimer) approximation, and E 0 = a 2 /4b is the depth of the potential well for the V (x) potential. For the four-minimum potential well described by equation (1), the quantitative value of the criterion can be slightly different.…”
The crystal structures and phonon spectra of orthorhombic cadmium titanate with the P bnm structure and of its two possible ferroelectrically distorted phases with P bn21 and P b21m space groups were calculated from first principles within the density functional theory. The obtained structural parameters and frequencies of Raman-and infrared-active modes are in good agreement with available experimental data for the P bnm phase. Expansion of the total energy in a Taylor series of two order parameters showed that the ground state of the system corresponds to the P bn21 structure into which the P bnm phase transforms through a second-order phase transition without intermediate phases. A substantial discrepancy between the calculated and experimentally observed lattice distortions and spontaneous polarization in the polar phase was explained by quantum fluctuations as well as by existence of twinning and competing long-period structures.
“…The lattice parameters and the equilibrium atomic positions were determined from the condition of decreasing of the residual forces acting on the atoms below 5 · 10 −6 Ha/Bohr (0.25 meV/Å) while the accuracy of the total energy calculation was better than 10 −10 Ha. To calculate of the phonon spectra, the formulas derived from the density functional perturbation theory and the interpolation technique 15 were used. The calculated lattice parameter for the cubic BaZrO 3 was a 0 = 4.1659Å and agreed well with the experimental value obtained at 10 K (4.191Å, Ref.…”
Section: Calculation and Experimental Techniquesmentioning
Phonon spectrum of cubic barium zirconate is calculated from first principles using the density functional theory. Unstable phonon mode with the R25 symmetry in the phonon spectrum indicates an instability of the cubic structure with respect to rotations of the oxygen octahedra. It is shown that the ground-state structure of the crystal is I4/mcm. In order to find the manifestations of the predicted instability, EXAFS measurements at the Ba LIII-edge are used to study the local structure of BaZrO3 at 300 K. An enhanced value of the Debye-Waller factor for the Ba-O atomic pair (σ 2 1 ∼ 0.015Å2 ) revealed in the experiment is associated with the predicted structural instability. The average amplitude of the thermal octahedra rotation estimated from the measured σ 2 1 value is ∼4 degrees at 300 K. The closeness of the calculated energies of different distorted phases resulting from the condensation of the R25 mode suggests a possible structural glass formation in BaZrO3 when lowering temperature, which explains the cause of the discrepancy between the calculations and experiment.
“…The pseudopotentials needed for calculations were constructed using the OPIUM program or borrowed from Ref. 18. The local structure of the solid solutions was modeled with CaF 2 and SrF 2 supercells containing 3×3×3 FCC unit cells in which one of 27 metal atoms was substituted by the Ba atom.…”
Section: A First-principles Calculationsmentioning
Spectral and kinetic properties of extrinsic crossluminescence (CL) in SrF 2 :Ba(1%) and CaF 2 :Ba(1%) are compared with those of intrinsic CL in BaF 2 and are analyzed taking into account EXAFS data obtained at the Ba L III edge and results of first-principles calculations. The CL decay time was revealed to be longer in SrF 2 :Ba and CaF 2 :Ba compared to BaF 2 . This fact contradicts the expected acceleration of luminescence decay which could result from an increased overlap of wave functions in solid solutions due to shortening of the Ba-F distance obtained in both EXAFS measurements and first-principles calculations. This discrepancy is explained by the effect of migration and subsequent non-radiative decay of the Ba (5p) core holes in BaF 2 and by decreasing of the probability of optical transitions between Ba (5p) states and the valence band in SrF 2 :Ba and CaF 2 :Ba predicted by first-principles calculations.
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