T. Voitenko, I. Fesych, S. Nedilko, O. Dziazko, M. Zelenko, A. O. Pilipenko, A. Slepets, K. Bychkov, D. Naumova
{"title":"Gd123亚微米粉末部分镧系元素取代的影响","authors":"T. Voitenko, I. Fesych, S. Nedilko, O. Dziazko, M. Zelenko, A. O. Pilipenko, A. Slepets, K. Bychkov, D. Naumova","doi":"10.1109/ELNANO.2018.8477474","DOIUrl":null,"url":null,"abstract":"<tex>$\\mathbf{GdLn}_{\\mathbf{x}}\\mathbf{Ba}_{2-\\mathbf{x}}\\mathbf{Cu}_{3}\\mathbf{O}_{\\mathbf{y}} (\\mathbf{Ln}=\\mathbf{La}, 0\\leq \\boldsymbol{x}\\leq 0.6;\\mathbf{Ln}=\\mathbf{Nd}, \\mathbf{Sm, Eu}, 0\\leq \\boldsymbol{x}\\leq 0.5)$</tex> (Gd123:Ln) samples were synthesized using the sol-gel method. The homogeneity region, variation of the crystal lattice and oxygen stoichiometry of the Gd123:Ln solid solutions were studied as a function of the substitution degree <tex>$\\boldsymbol{x}$</tex>. It was shown that the homogeneity region becomes wider when going from Eu<sup>3+</sup> <tex>$(\\boldsymbol{x}\\leq 0.35)$</tex> to La<sup>3</sup>+ <tex>$(\\boldsymbol{x}\\leq 0.5)$</tex>, but for all lanthanides the symmetry changes from orthorhombic to tetragonal for <tex>$\\boldsymbol{x}\\sim 0.05$</tex>. Measurements of the electrical resistance of Gd123:Ln samples in the temperature range 77–300 K revealed superconducting transition temperatures over 77 K only for <tex>$\\boldsymbol{x}=0$</tex> and <tex>$\\boldsymbol{x}=0.05$</tex>.","PeriodicalId":269665,"journal":{"name":"2018 IEEE 38th International Conference on Electronics and Nanotechnology (ELNANO)","volume":"45 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Effect of Partial Lanthanide Substitutions of Gd123 Submicronic Powder\",\"authors\":\"T. Voitenko, I. Fesych, S. Nedilko, O. Dziazko, M. Zelenko, A. O. Pilipenko, A. Slepets, K. Bychkov, D. Naumova\",\"doi\":\"10.1109/ELNANO.2018.8477474\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<tex>$\\\\mathbf{GdLn}_{\\\\mathbf{x}}\\\\mathbf{Ba}_{2-\\\\mathbf{x}}\\\\mathbf{Cu}_{3}\\\\mathbf{O}_{\\\\mathbf{y}} (\\\\mathbf{Ln}=\\\\mathbf{La}, 0\\\\leq \\\\boldsymbol{x}\\\\leq 0.6;\\\\mathbf{Ln}=\\\\mathbf{Nd}, \\\\mathbf{Sm, Eu}, 0\\\\leq \\\\boldsymbol{x}\\\\leq 0.5)$</tex> (Gd123:Ln) samples were synthesized using the sol-gel method. The homogeneity region, variation of the crystal lattice and oxygen stoichiometry of the Gd123:Ln solid solutions were studied as a function of the substitution degree <tex>$\\\\boldsymbol{x}$</tex>. It was shown that the homogeneity region becomes wider when going from Eu<sup>3+</sup> <tex>$(\\\\boldsymbol{x}\\\\leq 0.35)$</tex> to La<sup>3</sup>+ <tex>$(\\\\boldsymbol{x}\\\\leq 0.5)$</tex>, but for all lanthanides the symmetry changes from orthorhombic to tetragonal for <tex>$\\\\boldsymbol{x}\\\\sim 0.05$</tex>. Measurements of the electrical resistance of Gd123:Ln samples in the temperature range 77–300 K revealed superconducting transition temperatures over 77 K only for <tex>$\\\\boldsymbol{x}=0$</tex> and <tex>$\\\\boldsymbol{x}=0.05$</tex>.\",\"PeriodicalId\":269665,\"journal\":{\"name\":\"2018 IEEE 38th International Conference on Electronics and Nanotechnology (ELNANO)\",\"volume\":\"45 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-04-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2018 IEEE 38th International Conference on Electronics and Nanotechnology (ELNANO)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ELNANO.2018.8477474\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2018 IEEE 38th International Conference on Electronics and Nanotechnology (ELNANO)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ELNANO.2018.8477474","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Effect of Partial Lanthanide Substitutions of Gd123 Submicronic Powder
$\mathbf{GdLn}_{\mathbf{x}}\mathbf{Ba}_{2-\mathbf{x}}\mathbf{Cu}_{3}\mathbf{O}_{\mathbf{y}} (\mathbf{Ln}=\mathbf{La}, 0\leq \boldsymbol{x}\leq 0.6;\mathbf{Ln}=\mathbf{Nd}, \mathbf{Sm, Eu}, 0\leq \boldsymbol{x}\leq 0.5)$ (Gd123:Ln) samples were synthesized using the sol-gel method. The homogeneity region, variation of the crystal lattice and oxygen stoichiometry of the Gd123:Ln solid solutions were studied as a function of the substitution degree $\boldsymbol{x}$. It was shown that the homogeneity region becomes wider when going from Eu3+$(\boldsymbol{x}\leq 0.35)$ to La3+ $(\boldsymbol{x}\leq 0.5)$, but for all lanthanides the symmetry changes from orthorhombic to tetragonal for $\boldsymbol{x}\sim 0.05$. Measurements of the electrical resistance of Gd123:Ln samples in the temperature range 77–300 K revealed superconducting transition temperatures over 77 K only for $\boldsymbol{x}=0$ and $\boldsymbol{x}=0.05$.