Abstract
The temperature behavior of the dielectric response ehis(T) at a frequency of 1 kHz (110 K< T<300 K), δe(T)=[ehis(T)-eZFC(T)], and of the order parameter q(T), characterizing e(T) in a relaxor, is investigated for the relaxor Cd2Nb2O7 on samples with different thermal and electric histories in a dc field much weaker than the polarization saturation field. In a weak field (E dc=0.95 kV/cm), the behavior of δe(T) ∝ χnl changes in the region T f =184 K and the ehis(T) curves diverge monotonically at lower temperatures, indicating the development of the glassy state in the system. Analysis of the behavior of q(T) in the framework of the model of spin and dipole glasses shows that random interactions of polar microscopic regions in the presence of random fields play a dominating role in the phase formed below T f in the ZFC and FH/ZFC regimes. The relative contribution of random fields increases in the FC regime in a weak field and is manifested in the ZFH/FC regime both below and above T f .
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.