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Ferroelectric soft and central modes in perovskite ceramics and thin films
Jan PetzeltInstitute of Physics Acad. Sci. Czech Republic
Prague, Czech [email protected]
Normal vibrational modes
Normal modes (whose quanta are phonons) are plane-wave excitations consisting of specific linear combinations of small atomic displacements (vibrations), which in the case of harmonic lattice (vibrations of atoms in parabolic potentials) do not interact with each other.Number of phonon branches is equal to the number of vibrationaldegrees of freedom in one primitive unit cell, i.e. 3s, where s is the number of atoms in the unit cell. 3 of them are acoustic, remaining ones are optic.Symmetry classification of all phonons is according to irreducible representations of the corresponding crystal space group; Modes transforming according to one irreducible representation belong to one symmetry type (species). By symmetry arguments, they are linearly uncoupled from all other symmetry-types modes and obey the same selection rules (same activity in IR and Raman spectra).
Some useful keywords and concepts:
Mode degeneracy – given by the dimensionality of the corresponding ir. rep.: 3-dim – only in cubic structures (F (sometimes T) symbols)
2-dim – in optically uniaxial and cubic structures (E symbols)1-dim – everywhere (A and B symbols)
Transverse optical (TO) modes – IR active (polar) modesLongitudinal optical (LO) modes – do not couple with the el-mag
radiation, but can be evaluated from IR (or Raman) experimentSilent modes – in a given structure are inactive in any of the IR and
Raman spectraExclusion rule - in centro-symmetric structures no mode is both IR
and Raman activeTotally symmetric mode – the vibrational displacements do not break
the crystal symmetry (always 1-dim. ir. rep. with A symbol).Structural phase transitions – mostly change the symmetry ⇒ change
in selection rules and possibly in degeneracy (e.g. splitting if the symmetry reduces).
More general is factorized form (generalized 4-parameter oscillators, longitudinal damping γLO added), which reduces to Lyddanne-Sachs-Teller (L-S-T) relations for ω = 0. It is frequently used to fit the IR reflectivity.
Dielectric function of lattice vibrations (evaluated from the IR experiment)
The simplest model is sum of classical damped harmonic oscillators:
Both models display n complex poles and zeros whose frequency define the (complex) transverse and longitudinal normal modes, respectively. ωTOj andωLOj are moduli of these complex frequencies, respectively.
Simple perovskites
(a) Slater mode (b) Last mode (c) Axe modeFerroelectric soft mode Ferroelectric soft mode Highest frequencyin non-Pb perovskites in Pb-containing perovskites
IR active normal modes in simple cubic perovskites ABO3
A O B
SrTiO3 (ST)Incipient ferroelectric, at 105 K antiferrodistortive transition from simple cubic Pm3m structure to tetragonal phase I4/mcm.
Ferroelectric SM
Structural SM (doublet)
Mode frequencies in ST ceramics
(Petzelt et al., PRB 64, 184111 (2001))
x
y
z
TO1 (FE SM)(9-90) cm-1
TO2175 cm-1
TO4545 cm-1
Polar modes ( IR-active, R-inactive)
O2-
Sr2+
Ti4+
Below Ta ≈ 105 K - tetragonal symmetry
Cubic symmetry AFD SM –
non-polar Raman active
SrTiO3 – incipient ferroelectric
Antiferrodistortive (AFD) transition in SrTiO3 in R-point of the Brillouin zone
Eg
A1g Splitting of the AFD soft mode (Raman active below Ta)
Ta
Anisotropy of permittivity and splitting of the ferroelectric soft-mode in ST below the AFD transition
BaTiO3 (BT)
Factor-group analysis of the vibrational modes in different phases
Strong dielectric anisotropy in the tetragonal phase of BT single-domain crystal (Wemple et al., J. Phys. Chem. Solids 29, 1797 (1968), Camlibel et al., ibid. 31, 1417 (1969)).
Soft-mode in BaTiO3 crystal
0 200 400 600 800 1000 1200 14000
20406080
100120140160180200220240260280
CTR O
E
E
Freq
uenc
y (c
m-1)
Luspin_80 (IR refl.) Vogt_82 (HR) Laabidi_90 (R) Perry_65 (R) Burns_78 (R) Dougherty_94 (femt. ISRS)
Temperature (K)
B2
B1?
A1
F1u
TO1 mode in BaTiO3 single crystal
Temperature dependence of the overdamped soft-mode component in BaTiO3 .
Plotted is the equivalent Debye-relaxation frequency ω02/γ which corresponds
approximately to the maxima in ε”(ω) spectra.
87
BaTiO3 - rotational dispersion of long-wavelength IR phonon modes frequencies at room temperature
TO1(E)
TO2(E)
LO2(A) TO2(A)LO2(E)
TO3(E)TO1(A)LO3(E)
LO1(A)
TO4(E)LO1(E)TO4(E)TO4(A)
LO4(E)LO4(A)
k II c k ⊥ c
Extremely large A-E TO1 mode splitting ⇒ large dielectric anisotropy
Order-disorder model for BaTiO3 phase transitions
Ordered Ba
Dynamically disordered Ti
Chain-cluster structure proposed by Comes et al, Sol. State Commun. 6, 715 (1968):
Dipole-moment correlation of about 10-20 unit cells (4-8 nm) along the cubic crystal axes.