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g-C3N4纳米带的电子结构及光学性质的第一性原理计算
引用本文:杜秀娟,马柯榕,张政委,杨雯,张瑞,张清梅.g-C3N4纳米带的电子结构及光学性质的第一性原理计算[J].无机化学学报,2021,37(9):1674-1682.
作者姓名:杜秀娟  马柯榕  张政委  杨雯  张瑞  张清梅
作者单位:太原科技大学应用科学学院, 太原 030024;晋中学院化学化工系, 晋中 030619;太原科技大学材料科学与工程学院, 金属材料成型理论与技术山西省重点实验室, 太原 030024
基金项目:国家自然科学基金(No.51871158,11705124,11704274)资助。
摘    要:采用密度泛函理论的第一性原理方法研究了扶手椅型g-C3N4纳米带(AC-g-C3N4NRs)和锯齿型g-C3N4纳米带(ZZ-g-C3N4NRs)的电子结构和光学性质。结果表明:AC-g-C3N4NRs和ZZ-g-C3N4NRs的边缘H原子均能稳定存在。AC-g-C3N4NRs的价带顶主要由多数N原子贡献,而ZZ-g-C3N4NRs的价带顶主要由CH边缘附近的N原子贡献。AC-g-C3N4NRs的导带底主要属于纳米带一侧边缘或两侧边缘附近的C原子和N原子,而ZZ-g-C3N4NRs导带底主要属于ZZ-g-C3N4NRs的NH边缘附近的C原子和N原子。AC-g-C3N4NRs和ZZ-g-C3N4NRs的吸收系数和反射率都随纳米带宽度的增加而增加。随着AC-g-C3N4NR宽度的增加,吸收系数在低能区域产生明显的蓝移现象。

关 键 词:g-C3N4纳米带  结合能  电子结构  光学性质  第一性原理
收稿时间:2021/1/7 0:00:00
修稿时间:2021/6/17 0:00:00

First-Principles Calculations on Electronic Structures and Optical Properties of g-C3N4 Nanoribbons
DU Xiu-Juan,MA Ke-Rong,ZHANG Zheng-Wei,YANG Wen,ZHANG Rui,ZHANG Qing-Mei.First-Principles Calculations on Electronic Structures and Optical Properties of g-C3N4 Nanoribbons[J].Chinese Journal of Inorganic Chemistry,2021,37(9):1674-1682.
Authors:DU Xiu-Juan  MA Ke-Rong  ZHANG Zheng-Wei  YANG Wen  ZHANG Rui  ZHANG Qing-Mei
Institution:School of Applied Science, Taiyuan University of Science and Technology, Taiyuan 030024, China;Department of Chemistry and Chemical Engineering, Jinzhong University, Jinzhong, Shanxi 030619, China;Shanxi Key Laboratory of Metal Forming Theory and Technology, School of Material Science and Engineering, Taiyuan University of Science and Technology, Taiyuan 030024, China
Abstract:The first-principles method based on density functional theory was performed to investigate the electronic structure and optical properties of the armchair nanoribbons (AC-g-C3N4NRs) and zigzag g-C3N4 nanoribbons (ZZ-g-C3N4Rs). The results show that the edge H atoms of AC-g-C3N4NRs and ZZ-g-C3N4NRs can exist stably. The valence band maximums (VBMs) of AC-g-C3N4NRs are mainly contributed by most of N atoms, whereas the VBMs of ZZ-g-C3N4NRs are contributed by the N atoms near the CH edge. The conduction band minimums (CBMs) of AC-g-C3N4Rs mainly belong to C and N atoms near the one edge or two edges of AC-g-C3N4NRs, while the CBMs of ZZ-g-C3N4Rs mainly belong to C and N atoms near the NH edge of ZZ-g-C3N4NRs. The absorption coefficient and the reflectivity of AC-g-C3N4NR or ZZ-g-C3N4NR increased with the increasing width of the corresponding nanoribbon. An obvious blueshift phenomenon of the absorption coefficient could be generated in the low-energy range as the width of AC-g-C3N4NR increased.
Keywords:g-C3N4 nanoribbons  binding energies  electronic structure  optical properties  first-principles calculations
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