{"title":"通过掺杂镍调整纳米 Er2O3 的磁性、结构和屏蔽特性","authors":"Zein K. Heiba, Mohamed Bakr Mohamed, Ali Badawi","doi":"10.1149/2162-8777/ad71f1","DOIUrl":null,"url":null,"abstract":"We investigated the effects of Ni-doping amount on the structural, magnetic, and shielding properties of nano Er<sub>2</sub>O<sub>3</sub>. Nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> (x = 0, 0.05, 0.1, 0.15) samples were fabricated by a pechini scheme and characterized via X-ray diffraction. Rietveld refinement was used to discover the distribution of cations on the two crystallographic sites. Cation ordering in the two nonequivalent sites of the structure and the variation of the oxygen bond lengths of octahedra with the composition x were also investigated. A consistent reduction in the average bond lengths of (Er/Ni)O<sub>6</sub> octahedra around 8b and 24d as x progresses was observed. Average crystallite size reduced while average lattice micro-strain increased with increasing Ni doping. The correlation between magnetization and temperature for all samples under a magnetic field of 200 Oe was studied. Curie-Weiss law was applied to find the magnetic moments and the types of magnetic structure. The <italic toggle=\"yes\">μ</italic>\n<sub>eff</sub> in the Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples dropped from 9.7 to 9.36 μ<sub>B</sub> as the nickel doping level rose from 0 to 0.15. Calculated magnetic moments, <italic toggle=\"yes\">μ</italic>\n<sub>cal</sub>, were found to drop from 9.4 to 9.02 μ<sub>B</sub> as the nickel doping level changed from x = 0 to x = 0.15 in Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples. Curie paramagnetic temperature (<italic toggle=\"yes\">θ</italic>) for all samples has been observed to rise from −10.6 to −19.34. The theoretical gamma-ray attenuation parameters for nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples were acquired through the Phy-X/PSD software. The nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples have been proven to possess remarkable magnetic and neutron shielding applications.","PeriodicalId":11496,"journal":{"name":"ECS Journal of Solid State Science and Technology","volume":"30 1","pages":""},"PeriodicalIF":1.8000,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Tailoring the Magnetic, Structural and Shielding Characteristics of Nano Er2O3 via Ni Doping\",\"authors\":\"Zein K. Heiba, Mohamed Bakr Mohamed, Ali Badawi\",\"doi\":\"10.1149/2162-8777/ad71f1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We investigated the effects of Ni-doping amount on the structural, magnetic, and shielding properties of nano Er<sub>2</sub>O<sub>3</sub>. Nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> (x = 0, 0.05, 0.1, 0.15) samples were fabricated by a pechini scheme and characterized via X-ray diffraction. Rietveld refinement was used to discover the distribution of cations on the two crystallographic sites. Cation ordering in the two nonequivalent sites of the structure and the variation of the oxygen bond lengths of octahedra with the composition x were also investigated. A consistent reduction in the average bond lengths of (Er/Ni)O<sub>6</sub> octahedra around 8b and 24d as x progresses was observed. Average crystallite size reduced while average lattice micro-strain increased with increasing Ni doping. The correlation between magnetization and temperature for all samples under a magnetic field of 200 Oe was studied. Curie-Weiss law was applied to find the magnetic moments and the types of magnetic structure. The <italic toggle=\\\"yes\\\">μ</italic>\\n<sub>eff</sub> in the Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples dropped from 9.7 to 9.36 μ<sub>B</sub> as the nickel doping level rose from 0 to 0.15. Calculated magnetic moments, <italic toggle=\\\"yes\\\">μ</italic>\\n<sub>cal</sub>, were found to drop from 9.4 to 9.02 μ<sub>B</sub> as the nickel doping level changed from x = 0 to x = 0.15 in Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples. Curie paramagnetic temperature (<italic toggle=\\\"yes\\\">θ</italic>) for all samples has been observed to rise from −10.6 to −19.34. The theoretical gamma-ray attenuation parameters for nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples were acquired through the Phy-X/PSD software. The nano Er<sub>2−x</sub>Ni<sub>x</sub>O<sub>3</sub> samples have been proven to possess remarkable magnetic and neutron shielding applications.\",\"PeriodicalId\":11496,\"journal\":{\"name\":\"ECS Journal of Solid State Science and Technology\",\"volume\":\"30 1\",\"pages\":\"\"},\"PeriodicalIF\":1.8000,\"publicationDate\":\"2024-08-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ECS Journal of Solid State Science and Technology\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1149/2162-8777/ad71f1\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ECS Journal of Solid State Science and Technology","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1149/2162-8777/ad71f1","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
Tailoring the Magnetic, Structural and Shielding Characteristics of Nano Er2O3 via Ni Doping
We investigated the effects of Ni-doping amount on the structural, magnetic, and shielding properties of nano Er2O3. Nano Er2−xNixO3 (x = 0, 0.05, 0.1, 0.15) samples were fabricated by a pechini scheme and characterized via X-ray diffraction. Rietveld refinement was used to discover the distribution of cations on the two crystallographic sites. Cation ordering in the two nonequivalent sites of the structure and the variation of the oxygen bond lengths of octahedra with the composition x were also investigated. A consistent reduction in the average bond lengths of (Er/Ni)O6 octahedra around 8b and 24d as x progresses was observed. Average crystallite size reduced while average lattice micro-strain increased with increasing Ni doping. The correlation between magnetization and temperature for all samples under a magnetic field of 200 Oe was studied. Curie-Weiss law was applied to find the magnetic moments and the types of magnetic structure. The μeff in the Er2−xNixO3 samples dropped from 9.7 to 9.36 μB as the nickel doping level rose from 0 to 0.15. Calculated magnetic moments, μcal, were found to drop from 9.4 to 9.02 μB as the nickel doping level changed from x = 0 to x = 0.15 in Er2−xNixO3 samples. Curie paramagnetic temperature (θ) for all samples has been observed to rise from −10.6 to −19.34. The theoretical gamma-ray attenuation parameters for nano Er2−xNixO3 samples were acquired through the Phy-X/PSD software. The nano Er2−xNixO3 samples have been proven to possess remarkable magnetic and neutron shielding applications.
期刊介绍:
The ECS Journal of Solid State Science and Technology (JSS) was launched in 2012, and publishes outstanding research covering fundamental and applied areas of solid state science and technology, including experimental and theoretical aspects of the chemistry and physics of materials and devices.
JSS has five topical interest areas:
carbon nanostructures and devices
dielectric science and materials
electronic materials and processing
electronic and photonic devices and systems
luminescence and display materials, devices and processing.