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Annual Report 2012 - Latvijas Universitātes Cietvielu fizikas institūts

Annual Report 2012 - Latvijas Universitātes Cietvielu fizikas institūts

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Density and dielectric properties for different compositions<br />

Table 1<br />

Composition<br />

Density<br />

g/cm 3<br />

Dielectric<br />

permittivity ε<br />

(room T)<br />

Dielectric<br />

loss tanδ<br />

(room T)<br />

T max<br />

(C°)<br />

S4-1BT 4.51 1400 0.043 305 1.34<br />

S4-2BT 4.44 1240 0.652 270 1.45<br />

S4-4BT 4.34 1380 0.727 178 1.73<br />

S7-1BT 4.31 1800 0.100 245 1.39<br />

S7-2BT 4.34 940 0.490 211 1.57<br />

S7-4BT 4.43 1400 0.549 129 1.76<br />

PHASE TRANSITIONS AND PHYSICAL PROPERTIES IN<br />

Na 1/2 Bi 1/2 TiO 3 -BaTiO 3 SOLID SOLUTIONS<br />

M.Dunce, E.Birks, M.Antonova, A. Plaude, R. Ignatans<br />

Na 1/2 B 1/2 TiO 3 and its solid solutions attract interest mostly as an alternative for<br />

nowadays widely used lead-containing ferroelectric, use of which is gradually limited<br />

due to ecological considerations.<br />

Na 1/2 B 1/2 TiO 3 solid solutions with BaTiO 3 or (1-x)NBT-xBT show good<br />

piezoelectric properties. Most of the studies of (1-x)NBT-xBT are focused on the region<br />

around the morphotropic phase boundary, which is observed at BT concentration<br />

0.05≤x≤0.07. There is very little information about the compositions with higher BT<br />

content.<br />

In this work dielectric properties, polarization and x-ray diffraction are studied for<br />

NBT-BT solid solutions in a concentration range above the morphotropic phase<br />

boundary. Parameters, characterizing crystallographic structure and phase transition, are<br />

determined depending on the ratio of components of the solid solution. The results show<br />

that that all the studied compositions have tetragonal structure with maximal<br />

tetragonality slightly above the morphotropic phase boundary. In a wide concentration<br />

range ferroelectric relaxor properties are observed with a spontaneous transition to<br />

ferroelectric state at a temperature below the maximum of dielectric permittivity.<br />

Stability of the relaxor state decreases with increasing BaTiO 3 concentration, but only<br />

for compositions with low Na 1/2 Bi 1/2 TiO 3 content the normal ferroelectric-paraelectric<br />

phase transition, which is characteristic to pure BaTiO 3 , occurs. The change of<br />

diffuseness of the temperature dependence of dielectric permittivity is studied, using the<br />

power law. Attention is paid also to the concentration dependence of the thermal<br />

hysteresis. Mechanisms, which influence the change of the phase transition character<br />

and promote the appearance of the relaxor state, are discussed. The phase diagram of (1-<br />

x)Na 1/2 Bi 1/2 TiO 3 -xBaTiO 3 is revised.<br />

Special attention is paid to the phase coexistence region in the tetragonal side from<br />

the morphotropic phase boundary. The x-ray diffraction results show that the 1 st order<br />

ferroelectric phase transition, determined from a jump at temperature dependence of<br />

dielectric permittivity, is located inside the coexistence region of cubic and tetragonal<br />

phases and is below the temperature, where tetragonality disappears. At low BaTiO 3<br />

concentrations phase transition into ferroelectric state at cooling is slowly approached in<br />

time and is smeared over large temperature range. Rietveld method, applied for more<br />

precise evaluation of phase content, reveals large local deformations inside the<br />

ferroelectric phase.<br />

γ<br />

31

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