{"title":"Bi1-xSmxFeO3中以Sm取代Bi晶体结构转变的光谱表现及其磁性能","authors":"Evgen Leonenko , Andrii Yaremkevych , Maxim Rallev , Oleh Demianyk , Igor Fesych , Lesya Demchenko , Andrii Bodnaruk , Olena Fesenko","doi":"10.1016/j.rinma.2025.100768","DOIUrl":null,"url":null,"abstract":"<div><div>Nano-sized BiFeO<sub>3</sub>, BiFeO<sub>3</sub> doped with different amounts of Samarium, and SmFeO<sub>3</sub> were prepared by the solution combustion method. The obtained compounds have the general formula Bi<sub>1-x</sub>Sm<sub>x</sub>FeO<sub>3</sub>, where 0 ≤ x ≤ 0.2. To investigate and clarify the modifications in the crystal structure of the synthesized samples, X-ray diffraction, transmission electron microscopy, Raman spectroscopy, and Fourier-transform infrared spectroscopy were used. The compounds with gradual substitution of Bi<sup>3+</sup> by Sm<sup>3+</sup> are characterized by the sequence of the structural transformations from the rhombohedral phase <em>R</em>3<em>c</em> to the orthorhombic phase <em>Pbnm</em>. The concentration range corresponding to the coexistence of the rhombohedral (<em>R</em>3<em>c</em>) and orthorhombic (<em>Pbnm</em>) phases is observed in the interval 0.1 < x < 0.2. The compound Bi<sub>0.85</sub>Sm<sub>0.15</sub>FeO<sub>3</sub> has significant remanent magnetization, hysteresis loop and coercivity compared to other samples due to the coexistence of two crystalline phases orthorhombic (<em>Pbnm</em>) and rhombohedral (<em>R</em>3<em>c</em>) in a percentage ratio of 92 % and 8 %, i.e. a transformation of the crystalline phases occurs.</div></div>","PeriodicalId":101087,"journal":{"name":"Results in Materials","volume":"28 ","pages":"Article 100768"},"PeriodicalIF":0.0000,"publicationDate":"2025-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spectral manifestation of the transformation of the crystal structure with substituted Bi by Sm in Bi1-xSmxFeO3 and their magnetic properties\",\"authors\":\"Evgen Leonenko , Andrii Yaremkevych , Maxim Rallev , Oleh Demianyk , Igor Fesych , Lesya Demchenko , Andrii Bodnaruk , Olena Fesenko\",\"doi\":\"10.1016/j.rinma.2025.100768\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Nano-sized BiFeO<sub>3</sub>, BiFeO<sub>3</sub> doped with different amounts of Samarium, and SmFeO<sub>3</sub> were prepared by the solution combustion method. The obtained compounds have the general formula Bi<sub>1-x</sub>Sm<sub>x</sub>FeO<sub>3</sub>, where 0 ≤ x ≤ 0.2. To investigate and clarify the modifications in the crystal structure of the synthesized samples, X-ray diffraction, transmission electron microscopy, Raman spectroscopy, and Fourier-transform infrared spectroscopy were used. The compounds with gradual substitution of Bi<sup>3+</sup> by Sm<sup>3+</sup> are characterized by the sequence of the structural transformations from the rhombohedral phase <em>R</em>3<em>c</em> to the orthorhombic phase <em>Pbnm</em>. The concentration range corresponding to the coexistence of the rhombohedral (<em>R</em>3<em>c</em>) and orthorhombic (<em>Pbnm</em>) phases is observed in the interval 0.1 < x < 0.2. The compound Bi<sub>0.85</sub>Sm<sub>0.15</sub>FeO<sub>3</sub> has significant remanent magnetization, hysteresis loop and coercivity compared to other samples due to the coexistence of two crystalline phases orthorhombic (<em>Pbnm</em>) and rhombohedral (<em>R</em>3<em>c</em>) in a percentage ratio of 92 % and 8 %, i.e. a transformation of the crystalline phases occurs.</div></div>\",\"PeriodicalId\":101087,\"journal\":{\"name\":\"Results in Materials\",\"volume\":\"28 \",\"pages\":\"Article 100768\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2025-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Results in Materials\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2590048X2500113X\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Results in Materials","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2590048X2500113X","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
采用溶液燃烧法制备了纳米BiFeO3、掺杂不同量钐的BiFeO3和SmFeO3。所得化合物的通式为Bi1-xSmxFeO3,其中0≤x≤0.2。利用x射线衍射、透射电子显微镜、拉曼光谱和傅里叶变换红外光谱对合成样品的晶体结构进行了研究和澄清。Sm3+逐渐取代Bi3+的化合物,其结构由菱形相R3c转变为正交相Pbnm。在0.1 < x <; 0.2区间内观察到菱形相(R3c)和正交相(Pbnm)共存所对应的浓度范围。与其他样品相比,化合物Bi0.85Sm0.15FeO3具有显著的剩余磁化强度、磁滞回线和矫顽力,这是由于两种晶相分别以92%和8%的比例共存,即晶相发生了转变。
Spectral manifestation of the transformation of the crystal structure with substituted Bi by Sm in Bi1-xSmxFeO3 and their magnetic properties
Nano-sized BiFeO3, BiFeO3 doped with different amounts of Samarium, and SmFeO3 were prepared by the solution combustion method. The obtained compounds have the general formula Bi1-xSmxFeO3, where 0 ≤ x ≤ 0.2. To investigate and clarify the modifications in the crystal structure of the synthesized samples, X-ray diffraction, transmission electron microscopy, Raman spectroscopy, and Fourier-transform infrared spectroscopy were used. The compounds with gradual substitution of Bi3+ by Sm3+ are characterized by the sequence of the structural transformations from the rhombohedral phase R3c to the orthorhombic phase Pbnm. The concentration range corresponding to the coexistence of the rhombohedral (R3c) and orthorhombic (Pbnm) phases is observed in the interval 0.1 < x < 0.2. The compound Bi0.85Sm0.15FeO3 has significant remanent magnetization, hysteresis loop and coercivity compared to other samples due to the coexistence of two crystalline phases orthorhombic (Pbnm) and rhombohedral (R3c) in a percentage ratio of 92 % and 8 %, i.e. a transformation of the crystalline phases occurs.