{"title":"层状镍酸盐 Pr4Ni3-xCoxO8 用作高温超导体候选材料的中子衍射研究","authors":"Tomonori Miyatake, Yuki Wako, Ryota Abe, Satoru Tsukamoto, Masatomo Uehara","doi":"10.7566/jpsj.93.024709","DOIUrl":null,"url":null,"abstract":"Layered nickelate R<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub> (R = La, Pr, Nd, Sm) is a candidate for a high-temperature superconductor because its crystal structure and electronic state are very similar to high-temperature superconducting cuprates. We have performed carrier tuning by chemical substitution to Ni sites to bring the electronic states of Ni closer to that of Cu in superconducting cuprates. We aim to substitute the specific Ni sites for carrier tuning without disturbing the NiO<sub>2</sub> planes. In this study, we perform neutron powder diffraction experiments for the Pr<sub>4</sub>Ni<sub>3−</sub><i><sub>x</sub></i>Co<i><sub>x</sub></i>O<sub>8</sub> samples with doping Co for Ni sites to investigate the dopant distribution among the Ni sites. Rietveld analysis showed a tendency to preferentially occupy specific Ni sites when the doping level was low, but this is not the case for higher doping levels. We also analyzed the oxygen deficiency and found no oxygen deficiency in the NiO<sub>2</sub> planes with lower chemical substitutions, indicating that the relatively undisturbed conduction planes were maintained. Finally, we discuss the effects of Co doping into NiO<sub>2</sub> planes for the physical properties of R<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub>.","PeriodicalId":17304,"journal":{"name":"Journal of the Physical Society of Japan","volume":"397 2 1","pages":""},"PeriodicalIF":1.5000,"publicationDate":"2024-01-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Neutron Diffraction Study of Layered Nickelates Pr4Ni3−xCoxO8 for High-Temperature Superconductor Candidate\",\"authors\":\"Tomonori Miyatake, Yuki Wako, Ryota Abe, Satoru Tsukamoto, Masatomo Uehara\",\"doi\":\"10.7566/jpsj.93.024709\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Layered nickelate R<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub> (R = La, Pr, Nd, Sm) is a candidate for a high-temperature superconductor because its crystal structure and electronic state are very similar to high-temperature superconducting cuprates. We have performed carrier tuning by chemical substitution to Ni sites to bring the electronic states of Ni closer to that of Cu in superconducting cuprates. We aim to substitute the specific Ni sites for carrier tuning without disturbing the NiO<sub>2</sub> planes. In this study, we perform neutron powder diffraction experiments for the Pr<sub>4</sub>Ni<sub>3−</sub><i><sub>x</sub></i>Co<i><sub>x</sub></i>O<sub>8</sub> samples with doping Co for Ni sites to investigate the dopant distribution among the Ni sites. Rietveld analysis showed a tendency to preferentially occupy specific Ni sites when the doping level was low, but this is not the case for higher doping levels. We also analyzed the oxygen deficiency and found no oxygen deficiency in the NiO<sub>2</sub> planes with lower chemical substitutions, indicating that the relatively undisturbed conduction planes were maintained. Finally, we discuss the effects of Co doping into NiO<sub>2</sub> planes for the physical properties of R<sub>4</sub>Ni<sub>3</sub>O<sub>8</sub>.\",\"PeriodicalId\":17304,\"journal\":{\"name\":\"Journal of the Physical Society of Japan\",\"volume\":\"397 2 1\",\"pages\":\"\"},\"PeriodicalIF\":1.5000,\"publicationDate\":\"2024-01-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of the Physical Society of Japan\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.7566/jpsj.93.024709\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Physical Society of Japan","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.7566/jpsj.93.024709","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
层状镍酸盐 R4Ni3O8(R = La、Pr、Nd、Sm)是高温超导体的候选物质,因为它的晶体结构和电子状态与高温超导铜酸盐非常相似。我们通过对镍位点的化学置换进行了载流子调谐,使镍的电子状态更接近超导铜酸盐中铜的电子状态。我们的目标是在不干扰二氧化镍平面的情况下,替代特定的镍位点进行载流子调谐。在本研究中,我们对掺入 Co 的 Pr4Ni3-xCoxO8 样品进行了中子粉末衍射实验,以研究掺杂剂在 Ni 位点之间的分布。里特维尔德分析表明,当掺杂水平较低时,掺杂剂倾向于优先占据特定的镍位点,但当掺杂水平较高时,情况并非如此。我们还分析了缺氧情况,发现化学取代度较低的二氧化镍平面没有缺氧现象,这表明相对未受干扰的传导平面得以保持。最后,我们讨论了在 NiO2 平面中掺入 Co 对 R4Ni3O8 物理性质的影响。
Neutron Diffraction Study of Layered Nickelates Pr4Ni3−xCoxO8 for High-Temperature Superconductor Candidate
Layered nickelate R4Ni3O8 (R = La, Pr, Nd, Sm) is a candidate for a high-temperature superconductor because its crystal structure and electronic state are very similar to high-temperature superconducting cuprates. We have performed carrier tuning by chemical substitution to Ni sites to bring the electronic states of Ni closer to that of Cu in superconducting cuprates. We aim to substitute the specific Ni sites for carrier tuning without disturbing the NiO2 planes. In this study, we perform neutron powder diffraction experiments for the Pr4Ni3−xCoxO8 samples with doping Co for Ni sites to investigate the dopant distribution among the Ni sites. Rietveld analysis showed a tendency to preferentially occupy specific Ni sites when the doping level was low, but this is not the case for higher doping levels. We also analyzed the oxygen deficiency and found no oxygen deficiency in the NiO2 planes with lower chemical substitutions, indicating that the relatively undisturbed conduction planes were maintained. Finally, we discuss the effects of Co doping into NiO2 planes for the physical properties of R4Ni3O8.
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