Time–temperature superposition in the grain and grain boundary response regime of A2HoRuO6(A = Ba, Sr, Ca) double perovskite ceramics: a conductivity spectroscopic analysis
Abstract:The pursuit for an appropriate universal scaling factor to satisfy the time-temperature superposition principle for grain and grain boundary responses has been explored in the ac conductivity domain for polycrystalline double perovskite oxides A2HoRuO6 (AHR; A = Ba, Sr, Ca). The samples show different structural phases ranging from cubic to monoclinic with decreasing ionic radii. The degree of distortion in the materials is correlated to the strength of bonding through the bond valence sum (BVS). The conductiv… Show more
“…The long-range fundamental conductivity results in exact overlapping of the modulus and impedance peaks. [24][25][26][29][30][31][32][33][34] Especially, the investigation of electrical properties of these materials 27,28 can provide us an insight for their application in sensors, optical memory, electro-optic devices and actuations in the microelectromechanical systems etc.…”
“…The long-range fundamental conductivity results in exact overlapping of the modulus and impedance peaks. [24][25][26][29][30][31][32][33][34] Especially, the investigation of electrical properties of these materials 27,28 can provide us an insight for their application in sensors, optical memory, electro-optic devices and actuations in the microelectromechanical systems etc.…”
“…For disordered solids, this scaling characteristic is the time–temperature superposition principle (TTSP). 59,60 The scaling mechanism of experimental conductance isotherms is presented by a general formula: 61,62 where σ dc is the dc conductance, ν H is the hopping frequency and F is the temperature-independent function. The scaled conductance spectra for the synthesized compound at different temperatures are shown in Fig.…”
We have adopted two methods, sol–gel and solid-state synthesis methods to show the effect of grain size and the effect of temperature in the conductivity study.
“…The morphology and grain size are similar to that reported previously for Ba 2 HoRuO 6 . 25 The real part of dielectric permittivity 3 0 as a function of temperature T at selected test frequency f for Ba 2 PrRuO 6 between 10 K and 300 K are depicted in Fig. 2(a).…”
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