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首页> 外文期刊>Ferroelectrics: Letters Section >Frequency Dependent Dielectric Characteristics of Undoped and Vanadium-Doped SrBi_2Nb_2O_9 Ferroelectric Ceramics: A Comparative Study
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Frequency Dependent Dielectric Characteristics of Undoped and Vanadium-Doped SrBi_2Nb_2O_9 Ferroelectric Ceramics: A Comparative Study

机译:未掺杂和钒掺杂的SrBi_2Nb_2O_9铁电陶瓷的频率相关介电特性的比较研究

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The dielectric properties of undoped and vanadium (10 mol percent) doped SrBi_2Nb_2O_9 ferroelectric ceramics were studied in the 100 Hz to 1 MHz frequency range at various temperatures (300-823 K). The dielectric constants of vanadium doped ceramics were higher than those of undoped ceramics. A strong low frequency dielectric dispersion (LFDD) was encountered in these ceramics in the 573-823 K temperature range. The dispersion was stronger at low frequencies and higher temperatures for vanadium -doped ceramics. The dielectric constants measured in the wide frequency and temperature ranges for both the samples were found to fit well to the Jonscher's dielectric dispersion relations: epsilon_r' = epsilon_(infinity) + sin (n (T) pi/2) omega~(n(T)-1) a(T)/epsilon_o and epsilon_r" = sigma/epsilon_0 omega + cos (n (T) pi/2) omega~(n(T)-1) a(T)/epsilon_o. The lattice dielectric constant (epsilon_(infinity)) shows a peak at T_c. The coefficient A(T)( = a(T)S/L) and the exponent n (T) of the Jonscher's expression were, determined. The exponent n (T) was found to be minimum at the Curie temperature, T_c. The value of n for the vanadium-doped samples was less than that of the undoped one. The parameter A(T), which indicates the polarizing power, showed a prominent peak in the vicinity of the Curie temperature for both the samples. However, the value of A for the vanadium-doped samples was higher than that of undoped SBN ceramics.
机译:在100 Hz至1 MHz频率范围内(300-823 K)研究了未掺杂和钒(10摩尔%)掺杂的SrBi_2Nb_2O_9铁电陶瓷的介电性能。钒掺杂陶瓷的介电常数高于未掺杂陶瓷的介电常数。在573-823 K的温度范围内,这些陶瓷遇到了很强的低频介电弥散(LFDD)。对于钒掺杂的陶瓷,在低频和较高温度下,分散性更强。发现在两个样品的宽频率和温度范围内测得的介电常数与Jonscher的介电色散关系非常吻合:epsilon_r'= epsilon_(infinity)+ sin(n(T)pi / 2)ω〜(n( T)-1)a(T)/ epsilon_o和epsilon_r“ = sigma / epsilon_0ω+ cos(n(T)pi / 2)ω〜(n(T)-1)a(T)/ epsilon_o。晶格电介质常数(epsilon_(infinity))在T_c处出现一个峰值,确定了系数A(T)(= a(T)S / L)和Jonscher表达式的指数n(T)。发现在居里温度T_c处最小值最小,掺杂钒的样品的n值小于未掺杂样品的n值,指示极化功率的参数A(T)在样品中显示出一个明显的峰值。两个样品都居里温度附近,但是钒掺杂样品的A值比未掺杂SBN陶瓷的高。

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