Biswajit Jena, Dinesh Prajapati, Vishnu Shankar Rai, Harish Verma, Shail Upadhyay, N. B. Singh, Anup Kumar, D. Tiwary, K. D. Mandal
{"title":"掺钨Bi2/3Cu3Ti4O12陶瓷介电性能研究","authors":"Biswajit Jena, Dinesh Prajapati, Vishnu Shankar Rai, Harish Verma, Shail Upadhyay, N. B. Singh, Anup Kumar, D. Tiwary, K. D. Mandal","doi":"10.1007/s10854-025-14766-3","DOIUrl":null,"url":null,"abstract":"<div><p>Enhancing dielectric materials is crucial to the progress of energy storage technology. This work addresses the impacts of tungsten (W) substitution on the dielectric, electrical characteristics, and microstructure of ceramics called Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> (BCTO). The W-doped BCTO ceramics were fabricated employing a semi-wet method and sintered for eight hours at 1173 K. The synthesized Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4-x</sub>W<sub>x</sub>O<sub>12</sub> (<i>x</i> = 0.00, 0.05, 0.10, 0.20) labelled as BCTWO ceramics' phase development with minor secondary phase was validated by X-ray diffraction. X-ray photoelectron spectroscopy (XPS) was utilized to figure out the oxidation states of the elements, while energy-dispersive X-ray spectroscopy (EDX) analysis was employed to verify phase purity. The addition of a modest amount of W dopant decreased the grain size of BCTWO ceramics, most likely as a result of greater oxygen vacancy production during sintering, as shown by scanning electron microscopy (SEM) pictures. The surface texture was investigated by employing an atomic force microscope (AFM). The BCTO ceramic doped with tungsten (W) revealed an average grain size of 2.18 µm, which was greater than the un-doped BCTO ceramic. This could result in a higher dielectric constant (<i>ɛ</i>ʹ) and loss tangent (tan <i>δ</i>) in Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4-x</sub>W<sub>x</sub>O<sub>12</sub>(<i>x</i> = 0.05, 0.1, 0.2) ceramics. The BCTWO ceramic with higher dopant concentration was found to have a relatively high loss tangent (tan <i>δ</i> ~ 2.58 at 303 K and 1 kHz) and a high dielectric permittivity (<i>ε</i>ʹ ~ 7.8 × 10<sup>3</sup>).</p></div>","PeriodicalId":646,"journal":{"name":"Journal of Materials Science: Materials in Electronics","volume":"36 12","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2025-04-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Investigation of dielectric and electrical properties of tungsten doped Bi2/3Cu3Ti4O12 ceramics\",\"authors\":\"Biswajit Jena, Dinesh Prajapati, Vishnu Shankar Rai, Harish Verma, Shail Upadhyay, N. B. Singh, Anup Kumar, D. Tiwary, K. D. Mandal\",\"doi\":\"10.1007/s10854-025-14766-3\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Enhancing dielectric materials is crucial to the progress of energy storage technology. This work addresses the impacts of tungsten (W) substitution on the dielectric, electrical characteristics, and microstructure of ceramics called Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4</sub>O<sub>12</sub> (BCTO). The W-doped BCTO ceramics were fabricated employing a semi-wet method and sintered for eight hours at 1173 K. The synthesized Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4-x</sub>W<sub>x</sub>O<sub>12</sub> (<i>x</i> = 0.00, 0.05, 0.10, 0.20) labelled as BCTWO ceramics' phase development with minor secondary phase was validated by X-ray diffraction. X-ray photoelectron spectroscopy (XPS) was utilized to figure out the oxidation states of the elements, while energy-dispersive X-ray spectroscopy (EDX) analysis was employed to verify phase purity. The addition of a modest amount of W dopant decreased the grain size of BCTWO ceramics, most likely as a result of greater oxygen vacancy production during sintering, as shown by scanning electron microscopy (SEM) pictures. The surface texture was investigated by employing an atomic force microscope (AFM). The BCTO ceramic doped with tungsten (W) revealed an average grain size of 2.18 µm, which was greater than the un-doped BCTO ceramic. This could result in a higher dielectric constant (<i>ɛ</i>ʹ) and loss tangent (tan <i>δ</i>) in Bi<sub>2/3</sub>Cu<sub>3</sub>Ti<sub>4-x</sub>W<sub>x</sub>O<sub>12</sub>(<i>x</i> = 0.05, 0.1, 0.2) ceramics. The BCTWO ceramic with higher dopant concentration was found to have a relatively high loss tangent (tan <i>δ</i> ~ 2.58 at 303 K and 1 kHz) and a high dielectric permittivity (<i>ε</i>ʹ ~ 7.8 × 10<sup>3</sup>).</p></div>\",\"PeriodicalId\":646,\"journal\":{\"name\":\"Journal of Materials Science: Materials in Electronics\",\"volume\":\"36 12\",\"pages\":\"\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2025-04-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Materials Science: Materials in Electronics\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s10854-025-14766-3\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Materials Science: Materials in Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s10854-025-14766-3","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Investigation of dielectric and electrical properties of tungsten doped Bi2/3Cu3Ti4O12 ceramics
Enhancing dielectric materials is crucial to the progress of energy storage technology. This work addresses the impacts of tungsten (W) substitution on the dielectric, electrical characteristics, and microstructure of ceramics called Bi2/3Cu3Ti4O12 (BCTO). The W-doped BCTO ceramics were fabricated employing a semi-wet method and sintered for eight hours at 1173 K. The synthesized Bi2/3Cu3Ti4-xWxO12 (x = 0.00, 0.05, 0.10, 0.20) labelled as BCTWO ceramics' phase development with minor secondary phase was validated by X-ray diffraction. X-ray photoelectron spectroscopy (XPS) was utilized to figure out the oxidation states of the elements, while energy-dispersive X-ray spectroscopy (EDX) analysis was employed to verify phase purity. The addition of a modest amount of W dopant decreased the grain size of BCTWO ceramics, most likely as a result of greater oxygen vacancy production during sintering, as shown by scanning electron microscopy (SEM) pictures. The surface texture was investigated by employing an atomic force microscope (AFM). The BCTO ceramic doped with tungsten (W) revealed an average grain size of 2.18 µm, which was greater than the un-doped BCTO ceramic. This could result in a higher dielectric constant (ɛʹ) and loss tangent (tan δ) in Bi2/3Cu3Ti4-xWxO12(x = 0.05, 0.1, 0.2) ceramics. The BCTWO ceramic with higher dopant concentration was found to have a relatively high loss tangent (tan δ ~ 2.58 at 303 K and 1 kHz) and a high dielectric permittivity (εʹ ~ 7.8 × 103).
期刊介绍:
The Journal of Materials Science: Materials in Electronics is an established refereed companion to the Journal of Materials Science. It publishes papers on materials and their applications in modern electronics, covering the ground between fundamental science, such as semiconductor physics, and work concerned specifically with applications. It explores the growth and preparation of new materials, as well as their processing, fabrication, bonding and encapsulation, together with the reliability, failure analysis, quality assurance and characterization related to the whole range of applications in electronics. The Journal presents papers in newly developing fields such as low dimensional structures and devices, optoelectronics including III-V compounds, glasses and linear/non-linear crystal materials and lasers, high Tc superconductors, conducting polymers, thick film materials and new contact technologies, as well as the established electronics device and circuit materials.