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M. D. Glinchuk

Publications and source records attributed to M. D. Glinchuk.

38 records · Page 3Linked to original sources

Phase transitions in the antiferroelectric-ferroelectric mixed systems

Phase diagram of solid solutions of antiferroelectric and ferroelectric materials like PbZr$_{1-x}$Ti$_x$O$_3$ (PZT), Rb$_x$(NH$_4$)$_{1-x}$H$_2$PO$% _4$ (RADP) is calculated at the region $x\leq 0.1$. Antiferroelectric and ferroelectric order parameters (which correspond respectively to the difference and sum of two sublattices ions shifts) were introduced for antiferroelectric host lattice. Small admixture of ferroelectric component was considered as a random electric field source. The influence of this field on both aforementioned order parameters was calculated. Self consistent averaging with calculated random field distribution function made it possible to obtain the system of equations for order parameters of mixed system. The antiferroelectric $T_a$ and ferroelectric $T_c$ phase transition temperature concentrational dependence was expressed through the transition temperatures of the composition and members. The obtained $T_a(x)$ dependence was shown to fit pretty good the observed values for PZT and RADP. The application of the proposed theoretical approach to other types of mixed systems is discussed.

cond-mat.mtrl-sci↗

On the physical mechanisms of relaxation time distribution in disordered dielectrics

The distribution function of relaxation times in disordered dielectrics has been calculated in the random field theory framework. For this purpose, we first consider the dynamics of single two-orientable impurity electric dipole in a random electric field $E$ created by the rest of impurities in disordered ferroelectric. This dynamics is conveniently described by Langevin equation. Relaxation time $τ$ is then a reciprocal probability (calculated on the base of Fokker-Planck equation) of the dipole transition through barrier in a double-well potential (corresponding to two possible dipole orientations), distorted by a random fields. The obtained dependence $τ(E)$ made it possible to obtain the expression for relaxation times distribution function $F(τ)$(via random fields distribution function $f(E)$. Latter function has been calculated self-consistently in the random field theory framework. Nonlinear random field contribution and effects of spatial correlations between impurities have also been taken into account. It was shown that nonlinear contribution of random field gives asymmetric shape of $F(τ)$, while in linear case it is symmetric. Comparison of calculated $F(τ)$ curves with those extracted from empirical Cole-Cole (CC), Davidson-Cole (DC), Kohlrausch-William-Watts (KWW) and Havriliak-Negami (HN) functions had shown, that they correspond to mixed ferro-glass phase with coexistence of short and long-range order. Different forms of $F(τ)$ are determined by linear (CC) or nonlinear (DC, KWW, HN) contributions of random field.

cond-mat.mtrl-sci↗