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首页> 外文期刊>Journal of Sol-Gel Science and Technology >Investigations on the phase transition of Mn-doped BaTiO3 multifunctional ferroelectric ceramics through Raman, dielectric, and magnetic studies
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Investigations on the phase transition of Mn-doped BaTiO3 multifunctional ferroelectric ceramics through Raman, dielectric, and magnetic studies

机译:通过拉曼,电介质和磁力研究对Mn掺杂BATIO3多功能铁电陶瓷相变的研究

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摘要

BaTiO3 (BTO) and BaTi1-xMnxO3 (x=0.25, 0.50, 0.75mol%) ceramic materials have been prepared by the sol-gel combustion method. X-ray diffraction (XRD) has been carried out to characterize the phase purity and crystal structure of the prepared compounds, and all XRD patterns suggest tetragonal structure with the phase group of P4mm. The variation in the estimated lattice parameters confirms the incorporation of Mn atoms at Ti site of BTO. Raman spectroscopy studies under various temperatures suggest a phase transition from tetragonal to cubic phase at 433K, identified by a distinct Raman mode at 308cm(-1). As Raman modes are getting softened by Mn doping, phase transition temperature of the Mn-doped compounds is significantly decreased from 473K (x=0%) to 433K (x=0.75%). Dielectric properties such as permittivity and dielectric loss as the function of frequency under various temperatures have two distinct dielectric anomalies (i) at 393K associated to tetragonal to cubic phase transition and (ii) at 550K due to oxygen vacancy defect in the samples. Observation of weak ferromagnetism at 2, 300, and 400K in the M (H) and ZFC-FC curve, suppose its origin due to an intriguing exchange interaction between Mn and oxygen vacancies.
机译:通过溶胶 - 凝胶燃烧方法制备BatiO3(BTO)和Bati1-XMNXO3(x = 0.25,0.50,0.75mol%)陶瓷材料。已经进行了X射线衍射(XRD)以表征制备的化合物的相纯度和晶体结构,并且所有XRD图案都表达了具有P4mm的相组的四边形结构。估计的晶格参数的变化证实了在BTO的Ti位点掺入Mn原子。各种温度下拉曼光谱学研究表明,在433K时从四边形到立方相的相转变,通过308cm(-1)的不同拉曼模式鉴定。由于拉曼模式通过Mn掺杂软化,Mn掺杂化合物的相转变温度从473k(x = 0%)至433k(x = 0.75%)显着降低。随着各种温度下的频率函数的介电性质,例如介电常数和介电损耗具有两个不同的介电异常(I),其在393K处与四边形相位转移和(II)在550K中,由于样品中的氧空位缺陷,在550K处。在M(H)和ZFC-FC曲线中观察在2,300和400K处的弱铁磁性,假设其起源是由于Mn和氧空位之间的兴趣交换相互作用。

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