Nisha Kumari, Vishnu Saraswat, A. Dahshan, Neeraj Mehta
{"title":"通过加入过渡金属(铁、钴、镍、铜)调整二元 Se80Te20 玻璃的介电行为和直流导纳","authors":"Nisha Kumari, Vishnu Saraswat, A. Dahshan, Neeraj Mehta","doi":"10.1007/s10854-024-13801-z","DOIUrl":null,"url":null,"abstract":"<div><p>Transition metals (TMs) iron, cobalt, copper, and nickel have been chosen as the chemical modifiers with a binary alloy Se<sub>80</sub>Te<sub>20</sub> as the parent sample to make novel Se<sub>78</sub>Te<sub>20</sub>TM<sub>2</sub> (TM = Fe, Co, Ni, Cu) alloys. The frequency dependence of dielectric loss and a.c. conductivity (<span>\\({\\sigma }_{ac})\\)</span> have been studied and the possible mechanism has been checked. The dielectric constant (<i>ε</i>') shows significant variation among the samples, with the parent Se<sub>80</sub>Te<sub>20</sub> alloy exhibiting the highest value, followed closely by Se<sub>78</sub>Te<sub>20</sub>Cu<sub>2</sub>. Conversely, Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> and Se<sub>78</sub>Te<sub>20</sub>Ni<sub>2</sub> alloys exhibit much lower values. The dielectric loss also varies widely, with Se<sub>80</sub>Te<sub>20</sub>, while Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> and Se<sub>78</sub>Te<sub>20</sub>Ni<sub>2</sub> alloys present extremely low values of loss. The barrier height ranges between 0.31 eV (Fe-doped sample) and 1.2 eV (Ni-doped sample), indicating that doping influences the band gap significantly. The hooping distance shows considerable differences, with Fe-doped alloys exhibiting the highest value at 39.5 Å, while Co-doped samples show the lowest at 11.4 Å. Applicability of the Meyer-Neldel rule is observed in the a.c. conduction for all samples. The reducing nature of the power-law exponent “<i>s</i>” with increasing temperature indicates the correlated barrier hopping model for Se<sub>80</sub>Te<sub>20</sub> and Se<sub>78</sub>Te<sub>20</sub>TM<sub>2</sub> (TM = Co, Ni, Cu) alloys, as they exhibit a certain nature of variation. However, because “<i>s</i>” increases with temperature, the non-overlapping small polaron tunneling model is a particularly appropriate mechanism for a.c. conduction of ternary Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> alloy. Furthermore, we estimated the density of localized states for the synthesized material at various temperatures. The maximum reduction in the density of states is observed for the iron-containing parent sample.</p></div>","PeriodicalId":646,"journal":{"name":"Journal of Materials Science: Materials in Electronics","volume":"35 33","pages":""},"PeriodicalIF":2.8000,"publicationDate":"2024-11-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Tailoring of dielectric behavior and a.c. conduction in binary Se80Te20 glass by incorporation of transition metals (Fe, Co, Ni, Cu)\",\"authors\":\"Nisha Kumari, Vishnu Saraswat, A. Dahshan, Neeraj Mehta\",\"doi\":\"10.1007/s10854-024-13801-z\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Transition metals (TMs) iron, cobalt, copper, and nickel have been chosen as the chemical modifiers with a binary alloy Se<sub>80</sub>Te<sub>20</sub> as the parent sample to make novel Se<sub>78</sub>Te<sub>20</sub>TM<sub>2</sub> (TM = Fe, Co, Ni, Cu) alloys. The frequency dependence of dielectric loss and a.c. conductivity (<span>\\\\({\\\\sigma }_{ac})\\\\)</span> have been studied and the possible mechanism has been checked. The dielectric constant (<i>ε</i>') shows significant variation among the samples, with the parent Se<sub>80</sub>Te<sub>20</sub> alloy exhibiting the highest value, followed closely by Se<sub>78</sub>Te<sub>20</sub>Cu<sub>2</sub>. Conversely, Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> and Se<sub>78</sub>Te<sub>20</sub>Ni<sub>2</sub> alloys exhibit much lower values. The dielectric loss also varies widely, with Se<sub>80</sub>Te<sub>20</sub>, while Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> and Se<sub>78</sub>Te<sub>20</sub>Ni<sub>2</sub> alloys present extremely low values of loss. The barrier height ranges between 0.31 eV (Fe-doped sample) and 1.2 eV (Ni-doped sample), indicating that doping influences the band gap significantly. The hooping distance shows considerable differences, with Fe-doped alloys exhibiting the highest value at 39.5 Å, while Co-doped samples show the lowest at 11.4 Å. Applicability of the Meyer-Neldel rule is observed in the a.c. conduction for all samples. The reducing nature of the power-law exponent “<i>s</i>” with increasing temperature indicates the correlated barrier hopping model for Se<sub>80</sub>Te<sub>20</sub> and Se<sub>78</sub>Te<sub>20</sub>TM<sub>2</sub> (TM = Co, Ni, Cu) alloys, as they exhibit a certain nature of variation. However, because “<i>s</i>” increases with temperature, the non-overlapping small polaron tunneling model is a particularly appropriate mechanism for a.c. conduction of ternary Se<sub>78</sub>Te<sub>20</sub>Fe<sub>2</sub> alloy. Furthermore, we estimated the density of localized states for the synthesized material at various temperatures. The maximum reduction in the density of states is observed for the iron-containing parent sample.</p></div>\",\"PeriodicalId\":646,\"journal\":{\"name\":\"Journal of Materials Science: Materials in Electronics\",\"volume\":\"35 33\",\"pages\":\"\"},\"PeriodicalIF\":2.8000,\"publicationDate\":\"2024-11-22\",\"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/s10854-024-13801-z\",\"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/s10854-024-13801-z","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}
Tailoring of dielectric behavior and a.c. conduction in binary Se80Te20 glass by incorporation of transition metals (Fe, Co, Ni, Cu)
Transition metals (TMs) iron, cobalt, copper, and nickel have been chosen as the chemical modifiers with a binary alloy Se80Te20 as the parent sample to make novel Se78Te20TM2 (TM = Fe, Co, Ni, Cu) alloys. The frequency dependence of dielectric loss and a.c. conductivity (\({\sigma }_{ac})\) have been studied and the possible mechanism has been checked. The dielectric constant (ε') shows significant variation among the samples, with the parent Se80Te20 alloy exhibiting the highest value, followed closely by Se78Te20Cu2. Conversely, Se78Te20Fe2 and Se78Te20Ni2 alloys exhibit much lower values. The dielectric loss also varies widely, with Se80Te20, while Se78Te20Fe2 and Se78Te20Ni2 alloys present extremely low values of loss. The barrier height ranges between 0.31 eV (Fe-doped sample) and 1.2 eV (Ni-doped sample), indicating that doping influences the band gap significantly. The hooping distance shows considerable differences, with Fe-doped alloys exhibiting the highest value at 39.5 Å, while Co-doped samples show the lowest at 11.4 Å. Applicability of the Meyer-Neldel rule is observed in the a.c. conduction for all samples. The reducing nature of the power-law exponent “s” with increasing temperature indicates the correlated barrier hopping model for Se80Te20 and Se78Te20TM2 (TM = Co, Ni, Cu) alloys, as they exhibit a certain nature of variation. However, because “s” increases with temperature, the non-overlapping small polaron tunneling model is a particularly appropriate mechanism for a.c. conduction of ternary Se78Te20Fe2 alloy. Furthermore, we estimated the density of localized states for the synthesized material at various temperatures. The maximum reduction in the density of states is observed for the iron-containing parent sample.
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.