BaZr0.5Ti0.5O3: Lead-free relaxor ferroelectric or dipolar glass

被引:31
作者
Filipic, C. [1 ]
Kutnjak, Z. [1 ]
Pirc, R. [1 ]
Canu, G. [2 ]
Petzelt, J. [3 ]
机构
[1] Jozef Stefan Inst, Jamova Cesta 39, Ljubljana 1000, Slovenia
[2] CNR, Inst Energet & Interphases, Via De Marini 6, I-16149 Genoa, Italy
[3] Acad Sci Czech Republic, Inst Phys, Na Slovance 2, Prague 18221 8, Czech Republic
关键词
DYNAMICS; BAZRXTI1-XO3; RELAXATION; CERAMICS; SYSTEM;
D O I
10.1103/PhysRevB.93.224105
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Glassy freezing dynamics was investigated in BaZr0.5Ti0.5O3 (BZT50) ceramic samples by means of dielectric spectroscopy in the frequency range 0.001 Hz-1 MHz at temperatures 10 < T < 300 K. From measurements of the quasistatic dielectric polarization in bias electric fields up to similar to 28 kV/cm it has been found that a ferroelectric state cannot be induced, in contrast to the case of typical relaxors. This suggests that-at least for the above field amplitudes-BZT50 effectively behaves as a dipolar glass, which can be characterized by a negative value of the static third order nonlinear permittivity. The relaxation spectrum has been analyzed by means of the frequency-temperature plot, which shows that the longest relaxation time obeys the Vogel-Fulcher relation tau = tau(0) exp[E-0/(T - T-0)] with the freezing temperature of 48.1 K, whereas the corresponding value for the shortest relaxation time is similar to 0 K, implying an Arrhenius type behavior. By applying a standard expression for the static linear permittivity of dipolar glasses and/or relaxors the value of the Edwards-Anderson order parameter q(T) has been evaluated. It is further shown that q(T) can be described by the spherical random bond-random field model of relaxors.
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页数:8
相关论文
共 36 条
[1]   Finite-Temperature Properties of Ba(Zr, Ti)O3 Relaxors from First Principles [J].
Akbarzadeh, A. R. ;
Prosandeev, S. ;
Walter, Eric J. ;
Al-Barakaty, A. ;
Bellaiche, L. .
PHYSICAL REVIEW LETTERS, 2012, 108 (25)
[2]   Distribution of relaxation times of relaxors: comparison with dipolar glasses [J].
Banys, Juras ;
Grigalaitis, Robertas ;
Mikonis, Andrejus ;
Macutkevic, Jan ;
Keburis, Povilas .
PHYSICA STATUS SOLIDI C - CURRENT TOPICS IN SOLID STATE PHYSICS, VOL 6, NO 12, 2009, 6 (12) :2725-+
[3]   Common characteristics of displacive and relaxor ferroelectrics [J].
Bishop, A. R. ;
Bussmann-Holder, A. ;
Kamba, S. ;
Maglione, M. .
PHYSICAL REVIEW B, 2010, 81 (06)
[4]  
Blinc R., 2011, Advanced Ferroelectricity
[5]   The polarizability model for ferroelectricity in perovskite oxides [J].
Bussmann-Holder, Annette .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2012, 24 (27)
[6]   RELAXOR FERROELECTRICS: AN OVERVIEW [J].
Cross, L. Eric .
FERROELECTRICS, 1994, 151 (01) :305-320
[7]  
CROSS LE, 1987, FERROELECTRICS, V76, P241, DOI [10.1080/00150198708016945, 10.2109/jcersj.99.829]
[8]   A Raman and dielectric study of ferroelectric Ba(Ti1-xZrx)O3 ceramics [J].
Farhi, R ;
El Marssi, M ;
Simon, A ;
Ravez, J .
EUROPEAN PHYSICAL JOURNAL B, 1999, 9 (04) :599-604
[9]   The cluster glass route of relaxor ferroelectrics [J].
Kleemann, W. ;
Dec, J. ;
Miga, S. .
PHASE TRANSITIONS, 2015, 88 (03) :234-244
[10]   Crossover from ferroelectric to relaxor and cluster glass in BaTi1-xZrxO3 (x=0.25-0.35) studied by non-linear permittivity [J].
Kleemann, W. ;
Miga, S. ;
Dec, J. ;
Zhai, J. .
APPLIED PHYSICS LETTERS, 2013, 102 (23)