{"title":"MF/CuAl纳米复合材料的电磁性能","authors":"Khaled Roumaih","doi":"10.1515/zna-2023-0183","DOIUrl":null,"url":null,"abstract":"This study investigated the effects of CuAl<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (CuAl) on four types of spinel ferrites: CoFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (CoF), NiFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (NiF), MgFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (MgF), and ZnFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (ZnF) with regards to their electrical characteristics and microscopic magnetic behavior. According to the Seebeck coefficient (<jats:italic>φ</jats:italic>), the nanocomposites have a mixture of positive and negative charge carriers, except for CoF/CuAl, which has a positive charge carrier only. Depending on the temperature, the <jats:italic>DC</jats:italic> conductivity of all MF/CuAl nanocomposites has a conductor and semiconductor behavior. The dielectric properties were studied at different frequencies (100–10^8 Hz) and temperatures (300–673 K). The results demonstrated how temperature and frequency affect <jats:italic>AC</jats:italic> operating mechanisms. The high values of dielectric loss for all nanocomposites confirm their applicability in high-frequency microwave devices. The impedance study revealed that the equivalent circuit for all MF/CuAl nanocomposites is a mixture of R, L, and C. Temperature-magnetization graphs were obtained for all nanocomposites, indicating ferrimagnetic behavior except ZnF/CuAl. The magnetic transition temperature (<jats:italic>T</jats:italic> <jats:sub>Cm</jats:sub>), the Curie–Weiss constant (<jats:italic>θ</jats:italic> <jats:sub>CW</jats:sub>), and the effective magnetic moments (<jats:italic>μ</jats:italic> <jats:sub>eff</jats:sub>) for all nanocomposites were determined. The MF/CuAl samples were analyzed using ESR spectroscopy at room temperature. The spectra were distorted but remained distinct, potent, and sweeping. The <jats:italic>g</jats:italic>-factor values deviate from the free electron, which suggests that the Fe<jats:sup>3+</jats:sup>–O–Fe<jats:sup>3+</jats:sup> superexchange interaction has changed. In addition, the interaction effect between MF and CuAl is discussed.","PeriodicalId":23871,"journal":{"name":"Zeitschrift für Naturforschung A","volume":"40 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Electrical and magnetic properties of MF/CuAl nanocomposites\",\"authors\":\"Khaled Roumaih\",\"doi\":\"10.1515/zna-2023-0183\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This study investigated the effects of CuAl<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (CuAl) on four types of spinel ferrites: CoFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (CoF), NiFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (NiF), MgFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (MgF), and ZnFe<jats:sub>2</jats:sub>O<jats:sub>4</jats:sub> (ZnF) with regards to their electrical characteristics and microscopic magnetic behavior. According to the Seebeck coefficient (<jats:italic>φ</jats:italic>), the nanocomposites have a mixture of positive and negative charge carriers, except for CoF/CuAl, which has a positive charge carrier only. Depending on the temperature, the <jats:italic>DC</jats:italic> conductivity of all MF/CuAl nanocomposites has a conductor and semiconductor behavior. The dielectric properties were studied at different frequencies (100–10^8 Hz) and temperatures (300–673 K). The results demonstrated how temperature and frequency affect <jats:italic>AC</jats:italic> operating mechanisms. The high values of dielectric loss for all nanocomposites confirm their applicability in high-frequency microwave devices. The impedance study revealed that the equivalent circuit for all MF/CuAl nanocomposites is a mixture of R, L, and C. Temperature-magnetization graphs were obtained for all nanocomposites, indicating ferrimagnetic behavior except ZnF/CuAl. The magnetic transition temperature (<jats:italic>T</jats:italic> <jats:sub>Cm</jats:sub>), the Curie–Weiss constant (<jats:italic>θ</jats:italic> <jats:sub>CW</jats:sub>), and the effective magnetic moments (<jats:italic>μ</jats:italic> <jats:sub>eff</jats:sub>) for all nanocomposites were determined. The MF/CuAl samples were analyzed using ESR spectroscopy at room temperature. The spectra were distorted but remained distinct, potent, and sweeping. The <jats:italic>g</jats:italic>-factor values deviate from the free electron, which suggests that the Fe<jats:sup>3+</jats:sup>–O–Fe<jats:sup>3+</jats:sup> superexchange interaction has changed. In addition, the interaction effect between MF and CuAl is discussed.\",\"PeriodicalId\":23871,\"journal\":{\"name\":\"Zeitschrift für Naturforschung A\",\"volume\":\"40 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-11-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Zeitschrift für Naturforschung A\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1515/zna-2023-0183\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Zeitschrift für Naturforschung A","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1515/zna-2023-0183","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electrical and magnetic properties of MF/CuAl nanocomposites
This study investigated the effects of CuAl2O4 (CuAl) on four types of spinel ferrites: CoFe2O4 (CoF), NiFe2O4 (NiF), MgFe2O4 (MgF), and ZnFe2O4 (ZnF) with regards to their electrical characteristics and microscopic magnetic behavior. According to the Seebeck coefficient (φ), the nanocomposites have a mixture of positive and negative charge carriers, except for CoF/CuAl, which has a positive charge carrier only. Depending on the temperature, the DC conductivity of all MF/CuAl nanocomposites has a conductor and semiconductor behavior. The dielectric properties were studied at different frequencies (100–10^8 Hz) and temperatures (300–673 K). The results demonstrated how temperature and frequency affect AC operating mechanisms. The high values of dielectric loss for all nanocomposites confirm their applicability in high-frequency microwave devices. The impedance study revealed that the equivalent circuit for all MF/CuAl nanocomposites is a mixture of R, L, and C. Temperature-magnetization graphs were obtained for all nanocomposites, indicating ferrimagnetic behavior except ZnF/CuAl. The magnetic transition temperature (TCm), the Curie–Weiss constant (θCW), and the effective magnetic moments (μeff) for all nanocomposites were determined. The MF/CuAl samples were analyzed using ESR spectroscopy at room temperature. The spectra were distorted but remained distinct, potent, and sweeping. The g-factor values deviate from the free electron, which suggests that the Fe3+–O–Fe3+ superexchange interaction has changed. In addition, the interaction effect between MF and CuAl is discussed.